NPSMEFTd6 Class Reference

A model class for new physics in the form of the dimension-six effective Lagrangian. More...

#include <NPSMEFTd6.h>

Inheritance diagram for NPSMEFTd6:
[legend]
Collaboration diagram for NPSMEFTd6:
[legend]

Detailed Description

A model class for new physics in the form of the dimension-six effective Lagrangian.

Author
HEPfit Collaboration

This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to asumme lepton and quark flavour universality)

In this class we consider the dimension-six effective Lagrangian

\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]

The implementation is written in the basis of [88]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters containts 2 redundancies, given by coefficients \(C_{DHB} \) and \(C_{DHW} \), which correspond to operators not included in the basis of [88]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.

Initialization

After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().

Model parameters

The model parameters of NPSMEFTd6 are summarized below:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\).
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\).
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\).
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1_kk, CHL1_klr, CHL1_kli \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\).
CHL3_kk, CHL3_klr, CHL3_kli \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^j\big)\), for \(i,j=1,2,3\).
CHe_kk, CHe_klr, CHe_kli \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\).
CHQ1_kk, CHQ1_klr, CHQ1_kli \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\).
CHQ3_kk, CHQ3_klr, CHQ3_kli \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^j\big)\), for \(i,j=1,2,3\).
CHu_kk, CHu_klr, CHu_kli \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\).
CHd_kk, CHd_klr, CHd_kli \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CHud_klr, CHud_kli \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CeH_klr, CeH_kli \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\).
CuH_klr, CuH_kli \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\).
CdH_klr, CdH_kli \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\).
CuG_klr, CuG_kli \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CLL_1221, CLL_2112 \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.)
dg1Z \(\delta g_{1Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
dKappaga \(\delta \kappa_{\gamma}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
lambZ \(\lambda_{Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
eXint \(\varepsilon_{X}^{int}\) The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eXpar \(\varepsilon_{X}^{par}\) The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eVBFE_i \(\varepsilon_{VBF}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\)
eWHE_i \(\varepsilon_{WH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\)
eZHE_i \(\varepsilon_{ZH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\)
ettHE_i \(\varepsilon_{ttH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\)

Where the hermitian derivatives are defined as

\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]

and

\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\tau^a D_\mu - \overset{\leftarrow}{D}_\mu \tau^a)H. \]

Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\).
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\).
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\).
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1 \( (C_{HL}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal).
CHL3 \( (C_{HL}^{(3)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^i\big)\) (flavor universal).
CHe \( (C_{He})_{ii} \) The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal).
CHQ1 \( (C_{HQ}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal).
CHQ3 \( (C_{HQ}^{(3)})_{ii}\) The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^i\big)\) (flavor universal).
CHu \( (C_{Hu})_{ii} \) The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal).
CHd \( (C_{Hd})_{ii} \) The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CHud_r, CHud_i \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CeH_jjr, CeH_jji \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal).
CuH_jjr, CuH_jji \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal).
CdH_jjr, CdH_jji \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal).
CuG_klr, CuG_kli \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CLL \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.)

(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)

Model flags

The Flags of NPSMEFTd6 are summarized below:

Label Value Description
QuadraticTerms TRUE / FALSE This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized.
RotateCHWCHB TRUE / FALSE This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE.
PartialQFU TRUE / FALSE This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE.
FlavU3OfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
FlagUnivOfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
HiggsSM TRUE / FALSE This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE.
LoopHd6 TRUE / FALSE This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE.
LoopH3d6Quad TRUE / FALSE

This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE.

Important member functions

See the base classes of the current class.

Definition at line 753 of file NPSMEFTd6.h.

Public Member Functions

gslpp::complex AH_f (const double tau) const
 Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex AH_W (const double tau) const
 W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More...
 
gslpp::complex AHZga_f (const double tau, const double lambda) const
 Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex AHZga_W (const double tau, const double lambda) const
 W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double AuxObs_NP1 () const
 Auxiliary observable AuxObs_NP1 (See code for details.) More...
 
virtual double AuxObs_NP2 () const
 Auxiliary observable AuxObs_NP2 (See code for details.) More...
 
virtual double AuxObs_NP3 () const
 Auxiliary observable AuxObs_NP3 (See code for details.) More...
 
virtual double AuxObs_NP4 () const
 Auxiliary observable AuxObs_NP4 (See code for details.) More...
 
virtual double AuxObs_NP5 () const
 Auxiliary observable AuxObs_NP5 (See code for details.) More...
 
virtual double AuxObs_NP6 () const
 Auxiliary observable AuxObs_NP6 (See code for details.) More...
 
virtual double Br_H_exo () const
 The branching ratio of the of the Higgs into exotic particles. More...
 
virtual double Br_H_inv () const
 The branching ratio of the of the Higgs into invisible particles. More...
 
virtual double BrHbbRatio () const
 The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More...
 
virtual double BrHccRatio () const
 The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More...
 
virtual double BrHgagaRatio () const
 The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHggRatio () const
 The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More...
 
virtual double BrHmumuRatio () const
 The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtautauRatio () const
 The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtoinvRatio () const
 The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
 
virtual double BrHvisRatio () const
 The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
 
virtual double BrHWffRatio () const
 The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWjjRatio () const
 The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWlvRatio () const
 The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW2l2vRatio () const
 The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW4fRatio () const
 The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWW4jRatio () const
 The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWWRatio () const
 The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More...
 
virtual double BrHZddRatio () const
 The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZffRatio () const
 The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZgaeeRatio () const
 The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgallRatio () const
 The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZgamumuRatio () const
 The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgaRatio () const
 The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZllRatio () const
 The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZuuRatio () const
 The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZvvRatio () const
 The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ2e2muRatio () const
 The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4dRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4eRatio () const
 The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4fRatio () const
 The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZZ4lRatio () const
 The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4muRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4uRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4vRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZRatio () const
 The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double cgaga_HB () const
 The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cgg_HB () const
 The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual bool CheckParameters (const std::map< std::string, double > &DPars)
 A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More...
 
double CLL_bottom () const
 
double CLL_charm () const
 
double CLL_down () const
 
double CLL_mu () const
 
double CLL_strange () const
 
double CLL_tau () const
 
double CLL_up () const
 
double CLR_bottom () const
 
double CLR_charm () const
 
double CLR_down () const
 
double CLR_mu () const
 
double CLR_strange () const
 
double CLR_tau () const
 
double CLR_up () const
 
virtual double computeGammaTotalRatio () const
 The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
 
double CRL_bottom () const
 
double CRL_charm () const
 
double CRL_down () const
 
double CRL_mu () const
 
double CRL_strange () const
 
double CRL_tau () const
 
double CRL_up () const
 
double CRR_bottom () const
 
double CRR_charm () const
 
double CRR_down () const
 
double CRR_mu () const
 
double CRR_strange () const
 
double CRR_tau () const
 
double CRR_up () const
 
virtual double cZBox_HB () const
 The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZga_HB () const
 The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZZ_HB () const
 The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaa0 () const
 The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaa02 () const
 The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ () const
 The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ2 () const
 The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ () const
 The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ2 () const
 The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltacZ_HB () const
 The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaG1_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
 
virtual double deltaG1_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG1_hZARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG1_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
 
virtual double deltag1ZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
 
virtual double deltaG2_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
 
virtual double deltaG2_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
 
virtual double deltaG2_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
 
virtual double deltaG3_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
 
virtual double deltaG3_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
 
double deltag3G () const
 The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
 
gslpp::complex deltaG_Aff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Gff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hAA () const
 The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG_hAARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
gslpp::complex deltaG_hAff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual gslpp::complex deltaG_hff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
 
gslpp::complex deltaG_hGff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hgg () const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
 
virtual double deltaG_hggRatio () const
 The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG_hhhRatio () const
 The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
 
gslpp::complex deltaG_hZff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Zff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaGA_f (const Particle p) const
 New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double deltaGamma_W () const
 The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
 
virtual double deltaGamma_Wff (const Particle fi, const Particle fj) const
 The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
double deltaGammaHbbRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHbbRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHggRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
double deltaGammaHggRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
virtual double deltaGammaTotalRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
virtual double deltaGammaTotalRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
 
virtual double DeltaGF () const
 New physics contribution to the Fermi constant. More...
 
double deltaGL_f (const Particle p) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
virtual gslpp::complex deltaGL_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
gslpp::complex deltaGL_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
double deltaGL_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
 
virtual double deltaGmu () const
 The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaGmu2 () const
 The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
double deltaGR_f (const Particle p) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
virtual gslpp::complex deltaGR_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
gslpp::complex deltaGR_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
double deltaGR_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
 
virtual double deltaGV_f (const Particle p) const
 New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual double deltaGwd6 () const
 The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More...
 
virtual double deltaGwd62 () const
 The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More...
 
virtual double deltaGzd6 () const
 The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More...
 
virtual double deltaGzd62 () const
 The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More...
 
virtual double deltaKgammaNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
 
virtual double deltamb () const
 The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamb2 () const
 The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc () const
 The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc2 () const
 The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh () const
 The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh2 () const
 The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt () const
 The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt2 () const
 The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau () const
 The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau2 () const
 The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMwd6 () const
 The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More...
 
virtual double deltaMwd62 () const
 The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More...
 
virtual double deltaMz () const
 The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMz2 () const
 The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltayb_HB () const
 The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayc_HB () const
 The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaymu_HB () const
 The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayt_HB () const
 The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaytau_HB () const
 The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double dxseeWWdcos (const double sqrt_s, const double cos) const
 The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
 
virtual double dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
 The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
 
gslpp::complex f_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex g_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
double GammaHbbRatio () const
 The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
 
double GammaHccRatio () const
 The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
 
double GammaHgagaRatio () const
 The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHggRatio () const
 The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
 
double GammaHmumuRatio () const
 The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHtautauRatio () const
 The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
 
double GammaHWffRatio () const
 The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWjjRatio () const
 The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More...
 
double GammaHWlvRatio () const
 The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW2l2vRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW4fRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWW4jRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
double GammaHWWRatio () const
 The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
 
double GammaHZddRatio () const
 The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZeeRatio () const
 The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More...
 
double GammaHZffRatio () const
 The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZgaRatio () const
 The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHZllRatio () const
 The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZmumuRatio () const
 The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZuuRatio () const
 The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZvvRatio () const
 The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ2e2muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4dRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4eRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4fRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZZ4lRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4uRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4vRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZRatio () const
 The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double GammaW (const Particle fi, const Particle fj) const
 A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
 
virtual double GammaW () const
 The total width of the \(W\) boson, \(\Gamma_W\). More...
 
double getCed_1123 () const
 Return NP coeff Ced_1123. More...
 
double getCed_2223 () const
 Return NP coeff Ced_2223. More...
 
double getCeu_1133 () const
 Return NP coeff Ceu_1133. More...
 
double getCeu_2233 () const
 Return NP coeff Ceu_2233. More...
 
double getCHe_11 () const
 Return NP coeff CHe_11. More...
 
double getCHe_22 () const
 Return NP coeff CHe_22. More...
 
double getCHL1_11 () const
 Return NP coeff CHL1_11. More...
 
double getCHL1_22 () const
 Return NP coeff CHL1_22. More...
 
double getCHL3_11 () const
 Return NP coeff CHL3_11. More...
 
double getCHL3_22 () const
 Return NP coeff CHL3_22. More...
 
double getCLd_1123 () const
 Return NP coeff CLd_1123. More...
 
double getCLd_2223 () const
 Return NP coeff CLd_2223. More...
 
double getCLedQ_11 () const
 Return NP coeff CLedq_11. More...
 
double getCLedQ_22 () const
 Return NP coeff CLedq_22. More...
 
double getCLQ1_1123 () const
 Return NP coeff CLQ1_1123. More...
 
double getCLQ1_2223 () const
 Return NP coeff CLQ1_2223. More...
 
double getCLQ3_1123 () const
 Return NP coeff CLQ3_1123. More...
 
double getCLQ3_2223 () const
 Return NP coeff CLQ3_2223. More...
 
double getCLu_1133 () const
 Return NP coeff CLu_1133. More...
 
double getCLu_2233 () const
 Return NP coeff CLu_2233. More...
 
double getCpLedQ_11 () const
 Return NP coeff CpLedq_11. More...
 
double getCpLedQ_22 () const
 Return NP coeff CpLedq_22. More...
 
double getCQe_2311 () const
 Return NP coeff CQe_2322. More...
 
double getCQe_2322 () const
 Return NP coeff CQe_2322. More...
 
double getLambda_NP () const
 Return Lambda_NP. More...
 
virtual NPSMEFTd6MatchinggetMatching () const
 A method to get the Matching object for this model. More...
 
gslpp::complex I_triangle_1 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex I_triangle_2 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double kappaAeff () const
 The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
 
virtual double kappabeff () const
 The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
 
virtual double kappaceff () const
 The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
 
virtual double kappaGeff () const
 The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
 
virtual double kappamueff () const
 The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
 
virtual double kappataueff () const
 The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
 
virtual double kappaWeff () const
 The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
 
virtual double kappaZAeff () const
 The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
 
virtual double kappaZeff () const
 The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
 
virtual double lambdaZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
 
virtual double lambz_HB () const
 The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double mueeHvv (const double sqrt_s) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettH (const double sqrt_s) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBF (const double sqrt_s) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBF (const double sqrt_s) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZH (const double sqrt_s) const
 The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muepWBF (const double sqrt_s) const
 The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muepZBF (const double sqrt_s) const
 The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muggH (const double sqrt_s) const
 The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muggHH (const double sqrt_s) const
 The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...
 
virtual double muggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muggHpttH (const double sqrt_s) const
 The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double mummH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual double mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
 The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More...
 
virtual double muttH (const double sqrt_s) const
 The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muttHZbbboost (const double sqrt_s) const
 The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
 
virtual double muttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBF (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muVBFgamma (const double sqrt_s) const
 The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
 
virtual double muVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBFpVH (const double sqrt_s) const
 The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVH (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muWH (const double sqrt_s) const
 The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muZH (const double sqrt_s) const
 The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double Mw () const
 The mass of the \(W\) boson, \(M_W\). More...
 
 NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
 Constructor. More...
 
virtual double obliqueS () const
 The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More...
 
virtual double obliqueT () const
 The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More...
 
virtual double obliqueU () const
 The oblique parameter \(U\). More...
 
virtual double obliqueW () const
 The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More...
 
virtual double obliqueY () const
 The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More...
 
virtual bool PostUpdate ()
 The post-update method for NPSMEFTd6. More...
 
virtual double ppZHprobe (const double sqrt_s) const
 The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More...
 
virtual bool setFlag (const std::string name, const bool value)
 A method to set a flag of NPSMEFTd6. More...
 
virtual double xseeWW (const double sqrt_s) const
 Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
 
- Public Member Functions inherited from NPbase
virtual double A_f (const Particle f) const
 The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More...
 
virtual double AFB (const Particle f) const
 The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More...
 
virtual double BR_Zf (const Particle f) const
 The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
 
virtual double cbminuscc () const
 
virtual double cbminusctau () const
 
virtual double ccminusctau () const
 
virtual double cgaplusct () const
 
virtual double cgminuscga () const
 
virtual double cgplusct () const
 
virtual double cVpluscb () const
 
virtual double cVplusctau () const
 
virtual double deltaA_f (const Particle f) const
 The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
 
virtual double deltaAFB (const Particle f) const
 The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
 
virtual double deltaGamma_Z () const
 The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
 
virtual double deltaGamma_Zf (const Particle f) const
 The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
virtual double deltaN_nu () const
 The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
 
virtual double deltaR0_f (const Particle f) const
 The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More...
 
virtual double deltaR_inv () const
 The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
 
virtual double deltaSigmaHadron () const
 The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
 
virtual double deltaSin2thetaEff_e () const
 The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
 
virtual double deltaSin2thetaEff_mu () const
 The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
 
virtual gslpp::complex gA_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double Gamma_Z () const
 The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
 
virtual double Gamma_Zf (const Particle f) const
 The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
 
virtual StandardModel getTrueSM () const
 A method to return a StandardModel object from NPbase. More...
 
virtual gslpp::complex gV_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual gslpp::complex kappaZ_f (const Particle f) const
 The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
 
virtual double muggHgagaInt (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
 
virtual double muppHmumu (const double sqrt_s) const
 
virtual double muppHZga (const double sqrt_s) const
 
virtual double N_nu () const
 The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
 
 NPbase ()
 The default constructor. More...
 
virtual double R0_f (const Particle f) const
 The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More...
 
virtual double R_inv () const
 The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
 
virtual gslpp::complex rhoZ_f (const Particle f) const
 The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
 
virtual double sigma0_had () const
 The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
 
virtual double sin2thetaEff (const Particle f) const
 The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
 
virtual bool Update (const std::map< std::string, double > &DPars)
 The update method for NPbase. More...
 
virtual double UpperLimitZgammaA (const double sqrt_s) const
 
virtual double UpperLimitZgammaA13 (const double sqrt_s) const
 
virtual double UpperLimitZgammaC (const double sqrt_s) const
 
virtual double UpperLimitZgammaC13 (const double sqrt_s) const
 
- Public Member Functions inherited from StandardModel
double Ale (double mu, orders order, bool Nf_thr=true) const
 The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
 
double ale_OS (const double mu, orders order=FULLNLO) const
 The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
 
double alphaMz () const
 The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More...
 
double Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
 
double AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 
double Beta_e (int nm, unsigned int nf) const
 QED beta function coefficients - eq. (36) hep-ph/0512066. More...
 
double Beta_s (int nm, unsigned int nf) const
 QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
 
double c02 () const
 The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
 
virtual bool CheckFlags () const
 A method to check the sanity of the set of model flags. More...
 
bool checkSMparamsForEWPO ()
 A method to check whether the parameters relevant to the EWPO are updated. More...
 
double computeBrHtobb () const
 The Br \((H\to bb)\) in the Standard Model. More...
 
double computeBrHtocc () const
 The Br \((H\to cc)\) in the Standard Model. More...
 
double computeBrHtogaga () const
 The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
 
double computeBrHtogg () const
 The Br \((H\to gg)\) in the Standard Model. More...
 
double computeBrHtomumu () const
 The Br \((H\to \mu\mu)\) in the Standard Model. More...
 
double computeBrHtotautau () const
 The Br \((H\to \tau\tau)\) in the Standard Model. More...
 
double computeBrHtoWW () const
 The Br \((H\to WW)\) in the Standard Model. More...
 
double computeBrHtoZga () const
 The Br \((H\to Z\gamma)\) in the Standard Model. More...
 
double computeBrHtoZZ () const
 The Br \((H\to ZZ)\) in the Standard Model. More...
 
double computeBrHtoZZinv () const
 The Br \((H\to ZZ \to inv)\) in the Standard Model. More...
 
void ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
 A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
 
void ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
 A method to collect \(\Delta\rho\) computed via subclasses. More...
 
double computeGammaHgaga_tt () const
 The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_WW () const
 The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgg_bb () const
 The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tb () const
 The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tt () const
 The top loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHTotal () const
 The Higgs total width in the Standard Model. More...
 
double computeGammaHZga_tt () const
 The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_WW () const
 The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [94]. More...
 
double computeSigmaggH (const double sqrt_s) const
 The ggH cross section in the Standard Model. More...
 
double computeSigmaggH_bb (const double sqrt_s) const
 The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tb (const double sqrt_s) const
 The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tt (const double sqrt_s) const
 The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmattH (const double sqrt_s) const
 The ttH production cross section in the Standard Model. More...
 
double computeSigmaVBF (const double sqrt_s) const
 The VBF cross section in the Standard Model. More...
 
double computeSigmaWF (const double sqrt_s) const
 The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaWH (const double sqrt_s) const
 The WH production cross section in the Standard Model. More...
 
double computeSigmaZF (const double sqrt_s) const
 The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaZH (const double sqrt_s) const
 The ZH production cross section in the Standard Model. More...
 
double computeSigmaZWF (const double sqrt_s) const
 The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
 
virtual double cW2 (const double Mw_i) const
 The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
 
virtual double cW2 () const
 
double DeltaAlpha () const
 The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
 
double DeltaAlphaL5q () const
 The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
 
double DeltaAlphaLepton (const double s) const
 Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
 
double DeltaAlphaTop (const double s) const
 Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
 
virtual gslpp::complex deltaKappaZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
 
virtual double DeltaR () const
 The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
 
virtual double DeltaRbar () const
 The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
 
virtual gslpp::complex deltaRhoZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
 
virtual double epsilon1 () const
 The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
 
virtual double epsilon2 () const
 The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
 
virtual double epsilon3 () const
 The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
 
virtual double epsilonb () const
 The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
 
virtual double Gamma_had () const
 The hadronic decay width of the \(Z\) boson, \(\Gamma_{h}\). More...
 
virtual double Gamma_inv () const
 The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
 
virtual double GammaZ (const Particle f) const
 The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
 
double getAle () const
 A get method to retrieve the fine-structure constant \(\alpha\). More...
 
double getAlsMz () const
 A get method to access the value of \(\alpha_s(M_Z)\). More...
 
virtual double getCBd () const
 The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
 
virtual double getCBs () const
 The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
 
virtual double getCDMK () const
 The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
 
virtual double getCepsK () const
 The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
 
CKM getCKM () const
 A get method to retrieve the member object of type CKM. More...
 
double getDAle5Mz () const
 A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double getDelGammaZ () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
 
double getDelMw () const
 A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
 
double getDelR0b () const
 A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double getDelR0c () const
 A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double getDelR0l () const
 A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double getDelSigma0H () const
 A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
 
double getDelSin2th_b () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double getDelSin2th_l () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double getDelSin2th_q () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
std::string getFlagKappaZ () const
 A method to retrieve the model flag KappaZ. More...
 
std::string getFlagMw () const
 A method to retrieve the model flag Mw. More...
 
std::string getFlagRhoZ () const
 A method to retrieve the model flag RhoZ. More...
 
const FlavourgetFlavour () const
 
double getGF () const
 A get method to retrieve the Fermi constant \(G_\mu\). More...
 
int getIterationNo () const
 
Particle getLeptons (const QCD::lepton p) const
 A get method to retrieve the member object of a lepton. More...
 
virtual double getMHl () const
 A get method to retrieve the Higgs mass \(m_h\). More...
 
virtual double getmq (const QCD::quark q, const double mu) const
 
double getMuw () const
 A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
 
EWSMApproximateFormulaegetMyApproximateFormulae () const
 A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
 
EWSMcachegetMyEWSMcache () const
 A get method to retrieve the member pointer of type EWSMcache. More...
 
LeptonFlavourgetMyLeptonFlavour () const
 
EWSMOneLoopEWgetMyOneLoopEW () const
 A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
 
EWSMThreeLoopEWgetMyThreeLoopEW () const
 
EWSMThreeLoopEW2QCDgetMyThreeLoopEW2QCD () const
 
EWSMThreeLoopQCDgetMyThreeLoopQCD () const
 
EWSMTwoFermionsLEP2getMyTwoFermionsLEP2 () const
 A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...
 
EWSMTwoLoopEWgetMyTwoLoopEW () const
 
EWSMTwoLoopQCDgetMyTwoLoopQCD () const
 
double getMz () const
 A get method to access the mass of the \(Z\) boson \(M_Z\). More...
 
virtual double getPhiBd () const
 Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
 
virtual double getPhiBs () const
 Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
 
gslpp::matrix< gslpp::complexgetUPMNS () const
 A get method to retrieve the object of the PMNS matrix. More...
 
gslpp::matrix< gslpp::complexgetVCKM () const
 A get method to retrieve the CKM matrix. More...
 
gslpp::matrix< gslpp::complexgetYd () const
 A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
 
gslpp::matrix< gslpp::complexgetYe () const
 A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
 
gslpp::matrix< gslpp::complexgetYn () const
 A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
 
gslpp::matrix< gslpp::complexgetYu () const
 A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
 
virtual bool Init (const std::map< std::string, double > &DPars)
 A method to initialize the model parameters. More...
 
virtual bool InitializeModel ()
 A method to initialize the model. More...
 
bool IsFlagNoApproximateGammaZ () const
 A method to retrieve the model flag NoApproximateGammaZ. More...
 
bool IsFlagWithoutNonUniversalVC () const
 A method to retrieve the model flag WithoutNonUniversalVC. More...
 
virtual double LEP2AFBbottom (const double s) const
 
virtual double LEP2AFBcharm (const double s) const
 
virtual double LEP2AFBmu (const double s) const
 
virtual double LEP2AFBtau (const double s) const
 
virtual double LEP2Rbottom (const double s) const
 
virtual double LEP2Rcharm (const double s) const
 
virtual double LEP2sigmaBottom (const double s) const
 
virtual double LEP2sigmaCharm (const double s) const
 
virtual double LEP2sigmaHadron (const double s) const
 
virtual double LEP2sigmaMu (const double s) const
 
virtual double LEP2sigmaTau (const double s) const
 
virtual double Mw_tree () const
 The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
 
double MwbarFromMw (const double Mw) const
 A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
 
double MwFromMwbar (const double Mwbar) const
 A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
 
double Mzbar () const
 The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
 
virtual bool PreUpdate ()
 The pre-update method for StandardModel. More...
 
virtual double rho_GammaW (const Particle fi, const Particle fj) const
 EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
 
double s02 () const
 The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
 
void setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
 A set method to change the model flag CacheInStandardModel of StandardModel. More...
 
void setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
 
bool setFlagSigmaForAFB (const bool flagSigmaForAFB_i)
 
bool setFlagSigmaForR (const bool flagSigmaForR_i)
 
virtual bool setFlagStr (const std::string name, const std::string value)
 A method to set a flag of StandardModel. More...
 
 StandardModel ()
 The default constructor. More...
 
virtual double sW2 (const double Mw_i) const
 The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More...
 
double sW2 () const
 
virtual double v () const
 The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
 
virtual ~StandardModel ()
 The default destructor. More...
 
- Public Member Functions inherited from QCD
double AboveTh (const double mu) const
 The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
void addParameters (std::vector< std::string > params_i)
 A method to add parameters that are specific to only one set of observables. More...
 
virtual double Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double Als4 (const double mu) const
 The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More...
 
virtual double AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double AlsOLD (const double mu, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
double AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More...
 
double AlsWithLambda (const double mu, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More...
 
double BelowTh (const double mu) const
 The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
double Beta0 (const double nf) const
 The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta1 (const double nf) const
 The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta2 (const double nf) const
 The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta3 (const double nf) const
 The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
void CacheShift (double cache[][5], int n) const
 A member used to manage the caching for this class. More...
 
void CacheShift (int cache[][5], int n) const
 
orders FullOrder (orders order) const
 Return the FULLORDER enum corresponding to order. More...
 
double Gamma0 (const double nf) const
 The \(\gamma_0\) coefficient used to compute the running of a mass. More...
 
double Gamma1 (const double nf) const
 The \(\gamma_1\) coefficient used to compute the running of a mass. More...
 
double Gamma2 (const double nf) const
 The \(\gamma_2\) coefficient used to compute the running of a mass. More...
 
double getAlsM () const
 A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
 
BParameter getBBd () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
 
BParameter getBBs () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
 
BParameter getBD () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More...
 
BParameter getBK () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More...
 
BParameter getBKd1 () const
 
BParameter getBKd3 () const
 
double getCF () const
 A get method to access the Casimir factor of QCD. More...
 
double getMAls () const
 A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
 
Meson getMesons (const QCD::meson m) const
 A get method to access a meson as an object of the type Meson. More...
 
double getMtpole () const
 A get method to access the pole mass of the top quark. More...
 
double getMub () const
 A get method to access the threshold between five- and four-flavour theory in GeV. More...
 
double getMuc () const
 A get method to access the threshold between four- and three-flavour theory in GeV. More...
 
double getMut () const
 A get method to access the threshold between six- and five-flavour theory in GeV. More...
 
double getNc () const
 A get method to access the number of colours \(N_c\). More...
 
double getOptionalParameter (std::string name) const
 A method to get parameters that are specific to only one set of observables. More...
 
Particle getQuarks (const QCD::quark q) const
 A get method to access a quark as an object of the type Particle. More...
 
std::vector< std::string > getUnknownParameters ()
 A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...
 
void initializeBParameter (std::string name_i) const
 A method to initialize B Parameter and the corresponding meson. More...
 
void initializeMeson (QCD::meson meson_i) const
 A method to initialize a meson. More...
 
double logLambda (const double nf, orders order) const
 Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
 
double Mbar2Mp (const double mbar, const orders order=FULLNLO) const
 Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More...
 
double Mp2Mbar (const double mp, const orders order=FULLNLO) const
 Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
 
double Mrun (const double mu, const double m, const orders order=FULLNLO) const
 Computes a running quark mass \(m(\mu)\) from \(m(m)\). More...
 
double Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNLO) const
 Runs a quark mass from \(\mu_i\) to \(\mu_f\). More...
 
double Mrun4 (const double mu_f, const double mu_i, const double m) const
 The running of a mass with the number of flavours \(n_f = 4\). More...
 
double MS2DRqmass (const double MSscale, const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double MS2DRqmass (const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double Nf (const double mu) const
 The number of active flavour at scale \(\mu\). More...
 
double NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
 Threshold corrections in matching als(nf+1) with als(nf) from eq. (34) of hep-ph/0512060. More...
 
std::string orderToString (const orders order) const
 Converts an object of the enum type "orders" to the corresponding string. More...
 
 QCD ()
 Constructor. More...
 
void setNc (double Nc)
 A set method to change the number of colours \(N_c\). More...
 
void setOptionalParameter (std::string name, double value)
 A method to set the parameter value for the parameters that are specific to only one set of observables. More...
 
double Thresholds (const int i) const
 For accessing the active flavour threshold scales. More...
 
- Public Member Functions inherited from Model
std::string getModelName () const
 A method to fetch the name of the model. More...
 
const double & getModelParam (std::string name) const
 
bool isModelGeneralTHDM () const
 
bool isModelGeorgiMachacek () const
 
bool IsModelInitialized () const
 A method to check if the model is initialized. More...
 
bool isModelLinearized () const
 
bool isModelParam (std::string name) const
 
bool isModelSUSY () const
 
bool isModelTHDM () const
 
bool isModelTHDMW () const
 
bool IsUpdateError () const
 A method to check if there was any error in the model update process. More...
 
 Model ()
 The default constructor. More...
 
void setModelGeneralTHDM ()
 
void setModelGeorgiMachacek ()
 
void setModelInitialized (bool ModelInitialized)
 A set method to fix the failure or success of the initialization of the model. More...
 
void setModelLinearized (bool linearized=true)
 
void setModelName (const std::string name)
 A method to set the name of the model. More...
 
void setModelSUSY ()
 
void setModelTHDM ()
 
void setModelTHDMW ()
 
void setSliced (bool Sliced)
 
void setUpdateError (bool UpdateError)
 A set method to fix the update status as success or failure. More...
 
virtual ~Model ()
 The default destructor. More...
 

Static Public Attributes

static const int NNPSMEFTd6Vars = 400
 The number of the model parameters in NPSMEFTd6. More...
 
static const int NNPSMEFTd6Vars_LFU_QFU = 204
 The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More...
 
static const std::string NPSMEFTd6Vars [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6VarsRot [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More...
 
static const std::string NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More...
 
- Static Public Attributes inherited from StandardModel
static const double GeVminus2_to_nb = 389379.338
 
static const double Mw_error = 0.00001
 The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More...
 
static const int NSMvars = 26
 The number of the model parameters in StandardModel. More...
 
static const int NumSMParamsForEWPO = 33
 The number of the SM parameters that are relevant to the EW precision observables. More...
 
static std::string SMvars [NSMvars]
 A string array containing the labels of the model parameters in StandardModel. More...
 
- Static Public Attributes inherited from QCD
static const int NQCDvars = 11
 The number of model parameters in QCD. More...
 
static std::string QCDvars [NQCDvars]
 An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...
 

Protected Member Functions

gslpp::complex CfB_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More...
 
gslpp::complex CfG_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More...
 
gslpp::complex CfH_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
 
gslpp::complex CfW_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More...
 
double CHF1_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More...
 
double CHF3_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More...
 
double CHf_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More...
 
gslpp::complex CHud_diag (const Particle u) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More...
 
virtual void setParameter (const std::string name, const double &value)
 A method to set the value of a parameter of the model. More...
 
- Protected Member Functions inherited from StandardModel
double AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
double AFB_NoISR_q (const QCD::quark q_flavor, const double s) const
 
bool checkEWPOscheme (const std::string scheme) const
 A method to check if a given scheme name in string form is valid. More...
 
virtual void computeCKM ()
 The method to compute the CKM matrix. More...
 
virtual void computeYukawas ()
 The method to compute the Yukawa matrices. More...
 
double Delta_EWQCD (const QCD::quark q) const
 The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More...
 
double getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm133 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm167 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu130 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu136 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu161 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau130 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau136 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau161 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau207 (double x) const
 
double getIntegrand_dsigmaBox_bottom130 (double x) const
 
double getIntegrand_dsigmaBox_bottom133 (double x) const
 
double getIntegrand_dsigmaBox_bottom136 (double x) const
 
double getIntegrand_dsigmaBox_bottom161 (double x) const
 
double getIntegrand_dsigmaBox_bottom167 (double x) const
 
double getIntegrand_dsigmaBox_bottom172 (double x) const
 
double getIntegrand_dsigmaBox_bottom183 (double x) const
 
double getIntegrand_dsigmaBox_bottom189 (double x) const
 
double getIntegrand_dsigmaBox_bottom192 (double x) const
 
double getIntegrand_dsigmaBox_bottom196 (double x) const
 
double getIntegrand_dsigmaBox_bottom200 (double x) const
 
double getIntegrand_dsigmaBox_bottom202 (double x) const
 
double getIntegrand_dsigmaBox_bottom205 (double x) const
 
double getIntegrand_dsigmaBox_bottom207 (double x) const
 
double getIntegrand_dsigmaBox_charm130 (double x) const
 
double getIntegrand_dsigmaBox_charm133 (double x) const
 
double getIntegrand_dsigmaBox_charm136 (double x) const
 
double getIntegrand_dsigmaBox_charm161 (double x) const
 
double getIntegrand_dsigmaBox_charm167 (double x) const
 
double getIntegrand_dsigmaBox_charm172 (double x) const
 
double getIntegrand_dsigmaBox_charm183 (double x) const
 
double getIntegrand_dsigmaBox_charm189 (double x) const
 
double getIntegrand_dsigmaBox_charm192 (double x) const
 
double getIntegrand_dsigmaBox_charm196 (double x) const
 
double getIntegrand_dsigmaBox_charm200 (double x) const
 
double getIntegrand_dsigmaBox_charm202 (double x) const
 
double getIntegrand_dsigmaBox_charm205 (double x) const
 
double getIntegrand_dsigmaBox_charm207 (double x) const
 
double getIntegrand_dsigmaBox_down130 (double x) const
 
double getIntegrand_dsigmaBox_down133 (double x) const
 
double getIntegrand_dsigmaBox_down136 (double x) const
 
double getIntegrand_dsigmaBox_down161 (double x) const
 
double getIntegrand_dsigmaBox_down167 (double x) const
 
double getIntegrand_dsigmaBox_down172 (double x) const
 
double getIntegrand_dsigmaBox_down183 (double x) const
 
double getIntegrand_dsigmaBox_down189 (double x) const
 
double getIntegrand_dsigmaBox_down192 (double x) const
 
double getIntegrand_dsigmaBox_down196 (double x) const
 
double getIntegrand_dsigmaBox_down200 (double x) const
 
double getIntegrand_dsigmaBox_down202 (double x) const
 
double getIntegrand_dsigmaBox_down205 (double x) const
 
double getIntegrand_dsigmaBox_down207 (double x) const
 
double getIntegrand_dsigmaBox_mu130 (double x) const
 
double getIntegrand_dsigmaBox_mu133 (double x) const
 
double getIntegrand_dsigmaBox_mu136 (double x) const
 
double getIntegrand_dsigmaBox_mu161 (double x) const
 
double getIntegrand_dsigmaBox_mu167 (double x) const
 
double getIntegrand_dsigmaBox_mu172 (double x) const
 
double getIntegrand_dsigmaBox_mu183 (double x) const
 
double getIntegrand_dsigmaBox_mu189 (double x) const
 
double getIntegrand_dsigmaBox_mu192 (double x) const
 
double getIntegrand_dsigmaBox_mu196 (double x) const
 
double getIntegrand_dsigmaBox_mu200 (double x) const
 
double getIntegrand_dsigmaBox_mu202 (double x) const
 
double getIntegrand_dsigmaBox_mu205 (double x) const
 
double getIntegrand_dsigmaBox_mu207 (double x) const
 
double getIntegrand_dsigmaBox_strange130 (double x) const
 
double getIntegrand_dsigmaBox_strange133 (double x) const
 
double getIntegrand_dsigmaBox_strange136 (double x) const
 
double getIntegrand_dsigmaBox_strange161 (double x) const
 
double getIntegrand_dsigmaBox_strange167 (double x) const
 
double getIntegrand_dsigmaBox_strange172 (double x) const
 
double getIntegrand_dsigmaBox_strange183 (double x) const
 
double getIntegrand_dsigmaBox_strange189 (double x) const
 
double getIntegrand_dsigmaBox_strange192 (double x) const
 
double getIntegrand_dsigmaBox_strange196 (double x) const
 
double getIntegrand_dsigmaBox_strange200 (double x) const
 
double getIntegrand_dsigmaBox_strange202 (double x) const
 
double getIntegrand_dsigmaBox_strange205 (double x) const
 
double getIntegrand_dsigmaBox_strange207 (double x) const
 
double getIntegrand_dsigmaBox_tau130 (double x) const
 
double getIntegrand_dsigmaBox_tau133 (double x) const
 
double getIntegrand_dsigmaBox_tau136 (double x) const
 
double getIntegrand_dsigmaBox_tau161 (double x) const
 
double getIntegrand_dsigmaBox_tau167 (double x) const
 
double getIntegrand_dsigmaBox_tau172 (double x) const
 
double getIntegrand_dsigmaBox_tau183 (double x) const
 
double getIntegrand_dsigmaBox_tau189 (double x) const
 
double getIntegrand_dsigmaBox_tau192 (double x) const
 
double getIntegrand_dsigmaBox_tau196 (double x) const
 
double getIntegrand_dsigmaBox_tau200 (double x) const
 
double getIntegrand_dsigmaBox_tau202 (double x) const
 
double getIntegrand_dsigmaBox_tau205 (double x) const
 
double getIntegrand_dsigmaBox_tau207 (double x) const
 
double getIntegrand_dsigmaBox_up130 (double x) const
 
double getIntegrand_dsigmaBox_up133 (double x) const
 
double getIntegrand_dsigmaBox_up136 (double x) const
 
double getIntegrand_dsigmaBox_up161 (double x) const
 
double getIntegrand_dsigmaBox_up167 (double x) const
 
double getIntegrand_dsigmaBox_up172 (double x) const
 
double getIntegrand_dsigmaBox_up183 (double x) const
 
double getIntegrand_dsigmaBox_up189 (double x) const
 
double getIntegrand_dsigmaBox_up192 (double x) const
 
double getIntegrand_dsigmaBox_up196 (double x) const
 
double getIntegrand_dsigmaBox_up200 (double x) const
 
double getIntegrand_dsigmaBox_up202 (double x) const
 
double getIntegrand_dsigmaBox_up205 (double x) const
 
double getIntegrand_dsigmaBox_up207 (double x) const
 
double getIntegrand_sigmaWithISR_bottom130 (double x) const
 
double getIntegrand_sigmaWithISR_bottom133 (double x) const
 
double getIntegrand_sigmaWithISR_bottom136 (double x) const
 
double getIntegrand_sigmaWithISR_bottom161 (double x) const
 
double getIntegrand_sigmaWithISR_bottom167 (double x) const
 
double getIntegrand_sigmaWithISR_bottom172 (double x) const
 
double getIntegrand_sigmaWithISR_bottom183 (double x) const
 
double getIntegrand_sigmaWithISR_bottom189 (double x) const
 
double getIntegrand_sigmaWithISR_bottom192 (double x) const
 
double getIntegrand_sigmaWithISR_bottom196 (double x) const
 
double getIntegrand_sigmaWithISR_bottom200 (double x) const
 
double getIntegrand_sigmaWithISR_bottom202 (double x) const
 
double getIntegrand_sigmaWithISR_bottom205 (double x) const
 
double getIntegrand_sigmaWithISR_bottom207 (double x) const
 
double getIntegrand_sigmaWithISR_charm130 (double x) const
 
double getIntegrand_sigmaWithISR_charm133 (double x) const
 
double getIntegrand_sigmaWithISR_charm136 (double x) const
 
double getIntegrand_sigmaWithISR_charm161 (double x) const
 
double getIntegrand_sigmaWithISR_charm167 (double x) const
 
double getIntegrand_sigmaWithISR_charm172 (double x) const
 
double getIntegrand_sigmaWithISR_charm183 (double x) const
 
double getIntegrand_sigmaWithISR_charm189 (double x) const
 
double getIntegrand_sigmaWithISR_charm192 (double x) const
 
double getIntegrand_sigmaWithISR_charm196 (double x) const
 
double getIntegrand_sigmaWithISR_charm200 (double x) const
 
double getIntegrand_sigmaWithISR_charm202 (double x) const
 
double getIntegrand_sigmaWithISR_charm205 (double x) const
 
double getIntegrand_sigmaWithISR_charm207 (double x) const
 
double getIntegrand_sigmaWithISR_down130 (double x) const
 
double getIntegrand_sigmaWithISR_down133 (double x) const
 
double getIntegrand_sigmaWithISR_down136 (double x) const
 
double getIntegrand_sigmaWithISR_down161 (double x) const
 
double getIntegrand_sigmaWithISR_down167 (double x) const
 
double getIntegrand_sigmaWithISR_down172 (double x) const
 
double getIntegrand_sigmaWithISR_down183 (double x) const
 
double getIntegrand_sigmaWithISR_down189 (double x) const
 
double getIntegrand_sigmaWithISR_down192 (double x) const
 
double getIntegrand_sigmaWithISR_down196 (double x) const
 
double getIntegrand_sigmaWithISR_down200 (double x) const
 
double getIntegrand_sigmaWithISR_down202 (double x) const
 
double getIntegrand_sigmaWithISR_down205 (double x) const
 
double getIntegrand_sigmaWithISR_down207 (double x) const
 
double getIntegrand_sigmaWithISR_mu130 (double x) const
 
double getIntegrand_sigmaWithISR_mu136 (double x) const
 
double getIntegrand_sigmaWithISR_mu161 (double x) const
 
double getIntegrand_sigmaWithISR_mu172 (double x) const
 
double getIntegrand_sigmaWithISR_mu183 (double x) const
 
double getIntegrand_sigmaWithISR_mu189 (double x) const
 
double getIntegrand_sigmaWithISR_mu192 (double x) const
 
double getIntegrand_sigmaWithISR_mu196 (double x) const
 
double getIntegrand_sigmaWithISR_mu200 (double x) const
 
double getIntegrand_sigmaWithISR_mu202 (double x) const
 
double getIntegrand_sigmaWithISR_mu205 (double x) const
 
double getIntegrand_sigmaWithISR_mu207 (double x) const
 
double getIntegrand_sigmaWithISR_strange130 (double x) const
 
double getIntegrand_sigmaWithISR_strange133 (double x) const
 
double getIntegrand_sigmaWithISR_strange136 (double x) const
 
double getIntegrand_sigmaWithISR_strange161 (double x) const
 
double getIntegrand_sigmaWithISR_strange167 (double x) const
 
double getIntegrand_sigmaWithISR_strange172 (double x) const
 
double getIntegrand_sigmaWithISR_strange183 (double x) const
 
double getIntegrand_sigmaWithISR_strange189 (double x) const
 
double getIntegrand_sigmaWithISR_strange192 (double x) const
 
double getIntegrand_sigmaWithISR_strange196 (double x) const
 
double getIntegrand_sigmaWithISR_strange200 (double x) const
 
double getIntegrand_sigmaWithISR_strange202 (double x) const
 
double getIntegrand_sigmaWithISR_strange205 (double x) const
 
double getIntegrand_sigmaWithISR_strange207 (double x) const
 
double getIntegrand_sigmaWithISR_tau130 (double x) const
 
double getIntegrand_sigmaWithISR_tau136 (double x) const
 
double getIntegrand_sigmaWithISR_tau161 (double x) const
 
double getIntegrand_sigmaWithISR_tau172 (double x) const
 
double getIntegrand_sigmaWithISR_tau183 (double x) const
 
double getIntegrand_sigmaWithISR_tau189 (double x) const
 
double getIntegrand_sigmaWithISR_tau192 (double x) const
 
double getIntegrand_sigmaWithISR_tau196 (double x) const
 
double getIntegrand_sigmaWithISR_tau200 (double x) const
 
double getIntegrand_sigmaWithISR_tau202 (double x) const
 
double getIntegrand_sigmaWithISR_tau205 (double x) const
 
double getIntegrand_sigmaWithISR_tau207 (double x) const
 
double getIntegrand_sigmaWithISR_up130 (double x) const
 
double getIntegrand_sigmaWithISR_up133 (double x) const
 
double getIntegrand_sigmaWithISR_up136 (double x) const
 
double getIntegrand_sigmaWithISR_up161 (double x) const
 
double getIntegrand_sigmaWithISR_up167 (double x) const
 
double getIntegrand_sigmaWithISR_up172 (double x) const
 
double getIntegrand_sigmaWithISR_up183 (double x) const
 
double getIntegrand_sigmaWithISR_up189 (double x) const
 
double getIntegrand_sigmaWithISR_up192 (double x) const
 
double getIntegrand_sigmaWithISR_up196 (double x) const
 
double getIntegrand_sigmaWithISR_up200 (double x) const
 
double getIntegrand_sigmaWithISR_up202 (double x) const
 
double getIntegrand_sigmaWithISR_up205 (double x) const
 
double getIntegrand_sigmaWithISR_up207 (double x) const
 
double Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
double Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
double Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const
 
double Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const
 
double Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
double Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
double m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const
 
double RAq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More...
 
double resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
 A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double RVh () const
 The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More...
 
double RVq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More...
 
double SchemeToDouble (const std::string scheme) const
 A method to convert a given scheme name in string form into a floating-point number with double precision. More...
 
double sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
double sigma_NoISR_q (const QCD::quark q_flavor, const double s) const
 
double taub () const
 Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...
 
- Protected Member Functions inherited from QCD
double MassOfNf (int nf) const
 The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...
 

Protected Attributes

double aleMz
 The em constant at Mz. More...
 
double BrHexo
 The branching ratio of exotic (not invisible) Higgs decays. More...
 
double BrHinv
 The branching ratio of invisible Higgs decays. More...
 
double C2B
 The dimension-6 operator coefficient \(C_{2W}\). More...
 
double C2W
 The dimension-6 operator coefficient \(C_{2B}\). More...
 
double CdH_11i
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More...
 
double CdH_11r
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More...
 
double CdH_12i
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More...
 
double CdH_12r
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More...
 
double CdH_13i
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More...
 
double CdH_13r
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More...
 
double CdH_22i
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More...
 
double CdH_22r
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More...
 
double CdH_23i
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More...
 
double CdH_23r
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More...
 
double CdH_33i
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More...
 
double CdH_33r
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More...
 
double CDHB
 The dimension-6 operator coefficient \(C_{DHB}\). More...
 
double CDHW
 The dimension-6 operator coefficient \(C_{DHW}\). More...
 
double Ced_1111
 
double Ced_1122
 
double Ced_1123
 
double Ced_1132
 
double Ced_1133
 
double Ced_2211
 
double Ced_2223
 
double Ced_2232
 
double Ced_3311
 
double Ced_3323
 
double Ced_3332
 
double Cee_1111
 
double Cee_1122
 
double Cee_1133
 
double Cee_2211
 
double Cee_3311
 
double CeH_11i
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More...
 
double CeH_11r
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More...
 
double CeH_12i
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More...
 
double CeH_12r
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More...
 
double CeH_13i
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More...
 
double CeH_13r
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More...
 
double CeH_22i
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More...
 
double CeH_22r
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More...
 
double CeH_23i
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More...
 
double CeH_23r
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More...
 
double CeH_33i
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More...
 
double CeH_33r
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More...
 
double Ceu_1111
 
double Ceu_1122
 
double Ceu_1133
 
double Ceu_2211
 
double Ceu_2233
 
double Ceu_3311
 
double CG
 The dimension-6 operator coefficient \(C_{G}\). More...
 
double CH
 The dimension-6 operator coefficient \(C_{H}\). More...
 
double CHB
 The dimension-6 operator coefficient \(C_{HB}\). More...
 
double CHbox
 The dimension-6 operator coefficient \(C_{H\Box}\). More...
 
double CHD
 The dimension-6 operator coefficient \(C_{HD}\). More...
 
double CHd_11
 The dimension-6 operator coefficient \((C_{Hd})_{11}\). More...
 
double CHd_12i
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More...
 
double CHd_12r
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More...
 
double CHd_13i
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More...
 
double CHd_13r
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More...
 
double CHd_22
 The dimension-6 operator coefficient \((C_{Hd})_{22}\). More...
 
double CHd_23i
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More...
 
double CHd_23r
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More...
 
double CHd_33
 The dimension-6 operator coefficient \((C_{Hd})_{33}\). More...
 
double CHe_11
 The dimension-6 operator coefficient \((C_{He})_{11}\). More...
 
double CHe_12i
 The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More...
 
double CHe_12r
 The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More...
 
double CHe_13i
 The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More...
 
double CHe_13r
 The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More...
 
double CHe_22
 The dimension-6 operator coefficient \((C_{He})_{22}\). More...
 
double CHe_23i
 The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More...
 
double CHe_23r
 The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More...
 
double CHe_33
 The dimension-6 operator coefficient \((C_{He})_{33}\). More...
 
double CHG
 The dimension-6 operator coefficient \(C_{HG}\). More...
 
double CHL1_11
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More...
 
double CHL1_12i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More...
 
double CHL1_12r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More...
 
double CHL1_13i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More...
 
double CHL1_13r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More...
 
double CHL1_22
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More...
 
double CHL1_23i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More...
 
double CHL1_23r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More...
 
double CHL1_33
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More...
 
double CHL3_11
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More...
 
double CHL3_12i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_12r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_13i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_13r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_22
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More...
 
double CHL3_23i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_23r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_33
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More...
 
double CHQ1_11
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More...
 
double CHQ1_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More...
 
double CHQ1_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More...
 
double CHQ1_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More...
 
double CHQ1_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More...
 
double CHQ1_22
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More...
 
double CHQ1_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More...
 
double CHQ1_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More...
 
double CHQ1_33
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More...
 
double CHQ3_11
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More...
 
double CHQ3_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More...
 
double CHQ3_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More...
 
double CHQ3_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More...
 
double CHQ3_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More...
 
double CHQ3_22
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More...
 
double CHQ3_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More...
 
double CHQ3_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More...
 
double CHQ3_33
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More...
 
double cHSM
 Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More...
 
double CHu_11
 The dimension-6 operator coefficient \((C_{Hu})_{11}\). More...
 
double CHu_12i
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More...
 
double CHu_12r
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More...
 
double CHu_13i
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More...
 
double CHu_13r
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More...
 
double CHu_22
 The dimension-6 operator coefficient \((C_{Hu})_{22}\). More...
 
double CHu_23i
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More...
 
double CHu_23r
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More...
 
double CHu_33
 The dimension-6 operator coefficient \((C_{Hu})_{33}\). More...
 
double CHud_11i
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More...
 
double CHud_11r
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More...
 
double CHud_12i
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More...
 
double CHud_12r
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More...
 
double CHud_13i
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More...
 
double CHud_13r
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More...
 
double CHud_22i
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More...
 
double CHud_22r
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More...
 
double CHud_23i
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More...
 
double CHud_23r
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More...
 
double CHud_33i
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More...
 
double CHud_33r
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More...
 
double CHW
 The dimension-6 operator coefficient \(C_{HW}\). More...
 
double CHWB
 The dimension-6 operator coefficient \(C_{HWB}\). More...
 
double CHWHB_gaga
 The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More...
 
double CHWHB_gagaorth
 The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More...
 
double CLd_1111
 
double CLd_1122
 
double CLd_1123
 
double CLd_1132
 
double CLd_1133
 
double CLd_2211
 
double CLd_2223
 
double CLd_2232
 
double CLd_3311
 
double CLd_3323
 
double CLd_3332
 
double CLe_1111
 
double CLe_1122
 
double CLe_1133
 
double CLe_2211
 
double CLe_3311
 
double CLedQ_11
 
double CLedQ_22
 
double cLH3d62
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More...
 
double cLHd6
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More...
 
double CLL_1111
 
double CLL_1122
 
double CLL_1133
 
double CLL_1221
 
double CLL_1331
 
double CLL_2112
 
double CLL_2211
 
double CLL_3113
 
double CLL_3311
 
double CLQ1_1111
 
double CLQ1_1122
 
double CLQ1_1123
 
double CLQ1_1132
 
double CLQ1_1133
 
double CLQ1_1221
 
double CLQ1_1331
 
double CLQ1_2112
 
double CLQ1_2211
 
double CLQ1_2223
 
double CLQ1_2232
 
double CLQ1_3113
 
double CLQ1_3311
 
double CLQ1_3323
 
double CLQ1_3332
 
double CLQ3_1111
 
double CLQ3_1122
 
double CLQ3_1123
 
double CLQ3_1132
 
double CLQ3_1133
 
double CLQ3_1221
 
double CLQ3_1331
 
double CLQ3_2112
 
double CLQ3_2211
 
double CLQ3_2223
 
double CLQ3_2232
 
double CLQ3_3113
 
double CLQ3_3311
 
double CLQ3_3323
 
double CLQ3_3332
 
double CLu_1111
 
double CLu_1122
 
double CLu_1133
 
double CLu_2211
 
double CLu_2233
 
double CLu_3311
 
double CpLedQ_11
 
double CpLedQ_22
 
double CQe_1111
 
double CQe_1122
 
double CQe_1133
 
double CQe_2211
 
double CQe_2311
 
double CQe_2322
 
double CQe_2333
 
double CQe_3211
 
double CQe_3222
 
double CQe_3233
 
double CQe_3311
 
double CuB_11i
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More...
 
double CuB_11r
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More...
 
double CuB_12i
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More...
 
double CuB_12r
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More...
 
double CuB_13i
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More...
 
double CuB_13r
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More...
 
double CuB_22i
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More...
 
double CuB_22r
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More...
 
double CuB_23i
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More...
 
double CuB_23r
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More...
 
double CuB_33i
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More...
 
double CuB_33r
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More...
 
double CuG_11i
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More...
 
double CuG_11r
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More...
 
double CuG_12i
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More...
 
double CuG_12r
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More...
 
double CuG_13i
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More...
 
double CuG_13r
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More...
 
double CuG_22i
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More...
 
double CuG_22r
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More...
 
double CuG_23i
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More...
 
double CuG_23r
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More...
 
double CuG_33i
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More...
 
double CuG_33r
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More...
 
double CuH_11i
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More...
 
double CuH_11r
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More...
 
double CuH_12i
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More...
 
double CuH_12r
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More...
 
double CuH_13i
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More...
 
double CuH_13r
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More...
 
double CuH_22i
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More...
 
double CuH_22r
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More...
 
double CuH_23i
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More...
 
double CuH_23r
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More...
 
double CuH_33i
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More...
 
double CuH_33r
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More...
 
double CuW_11i
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More...
 
double CuW_11r
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More...
 
double CuW_12i
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More...
 
double CuW_12r
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More...
 
double CuW_13i
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More...
 
double CuW_13r
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More...
 
double CuW_22i
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More...
 
double CuW_22r
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More...
 
double CuW_23i
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More...
 
double CuW_23r
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More...
 
double CuW_33i
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More...
 
double CuW_33r
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More...
 
double CW
 The dimension-6 operator coefficient \(C_{W}\). More...
 
double cW2_tree
 The square of the tree level values for the cosine of the weak angle. More...
 
double cW_tree
 The tree level values for the cosine of the weak angle. More...
 
double delta_AA
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_AZ
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_h
 Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More...
 
double delta_ZZ
 Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More...
 
double dg1Z
 Independent contribution to aTGC. More...
 
double dGammaHTotR1
 
double dGammaHTotR2
 
double dKappaga
 Independent contribution to aTGC. More...
 
double dZH
 Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization. More...
 
double eeettHint
 Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeettHpar
 Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeeWBFint
 Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeWBFpar
 Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeZHint
 Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeeZHpar
 Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeMz
 The em coupling at Mz. More...
 
double eeMz2
 The em coupling squared (at Mz). More...
 
double eggFint
 Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eggFpar
 Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eHbbint
 Intrinsic relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHbbpar
 Parametric relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHccint
 Intrinsic relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHccpar
 Parametric relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHgagaint
 Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHgagapar
 Parametric relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHggint
 Intrinsic relative theoretical error in \(H \to g g\). More...
 
double eHggpar
 Parametric relative theoretical error in \(H \to g g\). More...
 
double eHmumuint
 Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHmumupar
 Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHtautauint
 Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHtautaupar
 Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHWWint
 Intrinsic relative theoretical error in \(H \to W W\). More...
 
double eHWWpar
 Parametric relative theoretical error in \(H \to W W\). More...
 
double eHZgaint
 Intrinsic relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZgapar
 Parametric relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZZint
 Intrinsic relative theoretical error in \(H \to Z Z\). More...
 
double eHZZpar
 Parametric relative theoretical error in \(H \to Z Z\). More...
 
double ettH_1314_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_1314_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_2_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_2_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_78_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettH_78_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettHint
 Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHpar
 Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double eVBF_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBFint
 Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVBFpar
 Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eWH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWHint
 Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHpar
 Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eZH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZHint
 Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHpar
 Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double g1_tree
 The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More...
 
double g2_tree
 The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More...
 
double GammaHTotR
 NP contributions and Total to Higgs width ratio with SM. More...
 
double gZdL
 
double gZdR
 The tree level value of the \(Z\bar{d}d\) couplings in the SM. More...
 
double gZlL
 
double gZlR
 The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More...
 
double gZuL
 
double gZuR
 The tree level value of the \(Z\bar{u}u\) couplings in the SM. More...
 
double gZvL
 The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More...
 
double Lambda_NP
 The new physics scale [GeV]. More...
 
double lambdaH_tree
 The SM tree level value of the scalar quartic coupling in the potential. More...
 
double LambdaNP2
 The square of the new physics scale [GeV \(^2\)]. More...
 
double lambZ
 Independent contribution to aTGC. More...
 
Matching< NPSMEFTd6Matching, NPSMEFTd6NPSMEFTd6M
 
double sW2_tree
 The square of the tree level values for the sine of the weak angle. More...
 
double sW_tree
 The tree level values for the sine of the weak angle. More...
 
double UevL
 The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More...
 
double v2
 The square of the EW vev. More...
 
double v2_over_LambdaNP2
 The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More...
 
double VudL
 The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More...
 
double Yukb
 SM d-quark Yukawas. More...
 
double Yukc
 
double Yukd
 
double Yuke
 
double Yukmu
 
double Yuks
 
double Yukt
 SM u-quark Yukawas. More...
 
double Yuktau
 SM lepton Yukawas. More...
 
double Yuku
 
- Protected Attributes inherited from NPbase
StandardModel trueSM
 
- Protected Attributes inherited from StandardModel
double A
 The CKM parameter \(A\) in the Wolfenstein parameterization. More...
 
double ale
 The fine-structure constant \(\alpha\). More...
 
double alpha21
 
double alpha31
 
double AlsMz
 The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
 
bool bSigmaForAFB
 
bool bSigmaForR
 
double dAle5Mz
 The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double delGammaZ
 The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More...
 
double delMw
 The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More...
 
double delR0b
 The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double delR0c
 The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double delR0l
 The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double delsigma0H
 The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More...
 
double delSin2th_b
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double delSin2th_l
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double delSin2th_q
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
double delta
 
double etab
 The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More...
 
bool flag_order [orders_EW_size]
 An array of internal flags controlling the inclusions of higher-order corrections. More...
 
bool flagLEP2 [NUMofLEP2RCs]
 
double gamma
 \(\gamma \) used as an input for FlagWolfenstein = FALSE More...
 
double GF
 The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
 
double lambda
 The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More...
 
Particle leptons [6]
 An array of Particle objects for the leptons. More...
 
double mHl
 The Higgs mass \(m_h\) in GeV. More...
 
double muw
 A matching scale \(\mu_W\) around the weak scale in GeV. More...
 
CKM myCKM
 An object of type CKM. More...
 
PMNS myPMNS
 
double Mz
 The mass of the \(Z\) boson in GeV. More...
 
bool requireCKM
 An internal flag to control whether the CKM matrix has to be recomputed. More...
 
bool requireYe
 An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...
 
bool requireYn
 An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...
 
double rhob
 The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More...
 
double s12
 
double s13
 
double s23
 
Flavour SMFlavour
 An object of type Flavour. More...
 
Matching< StandardModelMatching, StandardModelSMM
 An object of type Matching. More...
 
double Vcb
 \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vub
 \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vus
 \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
gslpp::matrix< gslpp::complexYd
 The Yukawa matrix of the down-type quarks. More...
 
gslpp::matrix< gslpp::complexYe
 The Yukawa matrix of the charged leptons. More...
 
gslpp::matrix< gslpp::complexYn
 The Yukawa matrix of the neutrinos. More...
 
gslpp::matrix< gslpp::complexYu
 The Yukawa matrix of the up-type quarks. More...
 
- Protected Attributes inherited from QCD
double AlsM
 The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More...
 
double CA
 
double CF
 
bool computemt
 Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More...
 
double dAdA_NA
 
double dFdA_NA
 
double dFdF_NA
 
double FBsoFBd
 The ratio \( F_{B_s}/F_{B_d} \) necessary to compute \( F_{B_s} \). More...
 
double MAls
 The mass scale in GeV at which the strong coupling measurement is provided. More...
 
double mtpole
 The pole mass of the top quark. More...
 
double mub
 The threshold between five- and four-flavour theory in GeV. More...
 
double muc
 The threshold between four- and three-flavour theory in GeV. More...
 
double mut
 The threshold between six- and five-flavour theory in GeV. More...
 
double NA
 
double Nc
 The number of colours. More...
 
Particle quarks [6]
 The vector of all SM quarks. More...
 
bool requireYd
 Switch for generating the Yukawa couplings to the down-type quarks. More...
 
bool requireYu
 Switch for generating the Yukawa couplings to the up-type quarks. More...
 
double TF
 
- Protected Attributes inherited from Model
bool isSliced
 A boolean set to true if the current istance is a slice of an extended object. More...
 
std::map< std::string, boost::reference_wrapper< const double > > ModelParamMap
 
bool UpdateError
 A boolean set to false if update is successful. More...
 

Private Attributes

bool FlagFlavU3OfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More...
 
bool FlagHiggsSM
 A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More...
 
const bool FlagLeptonUniversal
 An internal boolean flag that is true if assuming lepton flavour universality. More...
 
bool FlagLoopH3d6Quad
 A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More...
 
bool FlagLoopHd6
 A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More...
 
bool FlagPartialQFU
 A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More...
 
bool FlagQuadraticTerms
 A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More...
 
const bool FlagQuarkUniversal
 An internal boolean flag that is true if assuming quark flavour universality. More...
 
bool FlagRotateCHWCHB
 A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More...
 
bool FlagUnivOfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More...
 
gsl_integration_cquad_workspace * w_WW
 

Additional Inherited Members

- Public Types inherited from StandardModel
enum  LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs }
 
enum  orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size }
 An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...
 
- Public Types inherited from QCD
enum  lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON }
 An enum type for leptons. More...
 
enum  meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, MESON_END }
 An enum type for mesons. More...
 
enum  quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM }
 An enum type for quarks. More...
 

Constructor & Destructor Documentation

◆ NPSMEFTd6()

NPSMEFTd6::NPSMEFTd6 ( const bool  FlagLeptonUniversal_in = false,
const bool  FlagQuarkUniversal_in = false 
)

Constructor.

Parameters
[in]FlagLeptonUniversal_inan internal boolean flag that is true if assuming lepton flavour universality
[in]FlagQuarkUniversal_inan internal boolean flag that is true if assuming quark flavour universality

Definition at line 252 of file NPSMEFTd6.cpp.

253 : NPbase(), NPSMEFTd6M(*this), FlagLeptonUniversal(FlagLeptonUniversal_in), FlagQuarkUniversal(FlagQuarkUniversal_in)
254 {
257  throw std::runtime_error("Invalid arguments for NPSMEFTd6::NPSMEFTd6()");
258 
259  FlagQuadraticTerms = false;
260  FlagRotateCHWCHB = false;
261  FlagPartialQFU = false;
262  FlagFlavU3OfX = false;
263  FlagUnivOfX = false;
264  FlagHiggsSM = false;
265  FlagLoopHd6 = false;
266  FlagLoopH3d6Quad = false;
268 
269  w_WW = gsl_integration_cquad_workspace_alloc(100);
270 
272 
273  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CG", boost::cref(CG)));
274  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CW", boost::cref(CW)));
275  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("C2B", boost::cref(C2B)));
276  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("C2W", boost::cref(C2W)));
277  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHG", boost::cref(CHG)));
278  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHW", boost::cref(CHW)));
279  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHB", boost::cref(CHB)));
280  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHWHB_gaga", boost::cref(CHWHB_gaga)));
281  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHWHB_gagaorth", boost::cref(CHWHB_gagaorth)));
282  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CDHB", boost::cref(CDHB)));
283  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CDHW", boost::cref(CDHW)));
284  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHWB", boost::cref(CHWB)));
285  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHD", boost::cref(CHD)));
286  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHbox", boost::cref(CHbox)));
287  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CH", boost::cref(CH)));
288  if (FlagLeptonUniversal) {
289  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1", boost::cref(CHL1_11)));
290  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3", boost::cref(CHL3_11)));
291  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe", boost::cref(CHe_11)));
292  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11r", boost::cref(CeH_11r)));
293  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22r", boost::cref(CeH_22r)));
294  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33r", boost::cref(CeH_33r)));
295  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11i", boost::cref(CeH_11i)));
296  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22i", boost::cref(CeH_22i)));
297  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33i", boost::cref(CeH_33i)));
298  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL", boost::cref(CLL_1221)));
299  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Cee", boost::cref(Cee_1111)));
300  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe", boost::cref(CLe_1111)));
301  } else {
302  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_11", boost::cref(CHL1_11)));
303  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_12r", boost::cref(CHL1_12r)));
304  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_13r", boost::cref(CHL1_13r)));
305  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_22", boost::cref(CHL1_22)));
306  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_23r", boost::cref(CHL1_23r)));
307  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_33", boost::cref(CHL1_33)));
308  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_12i", boost::cref(CHL1_12i)));
309  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_13i", boost::cref(CHL1_13i)));
310  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_23i", boost::cref(CHL1_23i)));
311  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_11", boost::cref(CHL3_11)));
312  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_12r", boost::cref(CHL3_12r)));
313  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_13r", boost::cref(CHL3_13r)));
314  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_22", boost::cref(CHL3_22)));
315  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_23r", boost::cref(CHL3_23r)));
316  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_33", boost::cref(CHL3_33)));
317  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_12i", boost::cref(CHL3_12i)));
318  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_13i", boost::cref(CHL3_13i)));
319  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_23i", boost::cref(CHL3_23i)));
320  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_11", boost::cref(CHe_11)));
321  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_12r", boost::cref(CHe_12r)));
322  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_13r", boost::cref(CHe_13r)));
323  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_22", boost::cref(CHe_22)));
324  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_23r", boost::cref(CHe_23r)));
325  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_33", boost::cref(CHe_33)));
326  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_12i", boost::cref(CHe_12i)));
327  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_13i", boost::cref(CHe_13i)));
328  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_23i", boost::cref(CHe_23i)));
329  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11r", boost::cref(CeH_11r)));
330  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_12r", boost::cref(CeH_12r)));
331  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_13r", boost::cref(CeH_13r)));
332  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22r", boost::cref(CeH_22r)));
333  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_23r", boost::cref(CeH_23r)));
334  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33r", boost::cref(CeH_33r)));
335  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11i", boost::cref(CeH_11i)));
336  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_12i", boost::cref(CeH_12i)));
337  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_13i", boost::cref(CeH_13i)));
338  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22i", boost::cref(CeH_22i)));
339  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_23i", boost::cref(CeH_23i)));
340  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33i", boost::cref(CeH_33i)));
341  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1111", boost::cref(CLL_1111)));
342  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1221", boost::cref(CLL_1221)));
343  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1122", boost::cref(CLL_1122)));
344  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1331", boost::cref(CLL_1331)));
345  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1133", boost::cref(CLL_1133)));
346  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Cee_1111", boost::cref(Cee_1111)));
347  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Cee_1122", boost::cref(Cee_1122)));
348  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Cee_1133", boost::cref(Cee_1133)));
349  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe_1111", boost::cref(CLe_1111)));
350  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe_1122", boost::cref(CLe_1122)));
351  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe_2211", boost::cref(CLe_2211)));
352  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe_1133", boost::cref(CLe_1133)));
353  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLe_3311", boost::cref(CLe_3311)));
354  }
355  if (FlagQuarkUniversal) {
356  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1", boost::cref(CHQ1_11)));
357  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3", boost::cref(CHQ3_11)));
358  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu", boost::cref(CHu_11)));
359  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd", boost::cref(CHd_11)));
360  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_r", boost::cref(CHud_11r)));
361  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_i", boost::cref(CHud_11i)));
362  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11r", boost::cref(CuH_11r)));
363  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22r", boost::cref(CuH_22r)));
364  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33r", boost::cref(CuH_33r)));
365  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11i", boost::cref(CuH_11i)));
366  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22i", boost::cref(CuH_22i)));
367  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33i", boost::cref(CuH_33i)));
368  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11r", boost::cref(CdH_11r)));
369  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22r", boost::cref(CdH_22r)));
370  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33r", boost::cref(CdH_33r)));
371  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11i", boost::cref(CdH_11i)));
372  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22i", boost::cref(CdH_22i)));
373  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33i", boost::cref(CdH_33i)));
374  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_r", boost::cref(CuG_11r)));
375  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_i", boost::cref(CuG_11i)));
376  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_r", boost::cref(CuW_11r)));
377  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_i", boost::cref(CuW_11i)));
378  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_r", boost::cref(CuB_11r)));
379  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_i", boost::cref(CuB_11i)));
380  } else {
381  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_11", boost::cref(CHQ1_11)));
382  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_12r", boost::cref(CHQ1_12r)));
383  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_13r", boost::cref(CHQ1_13r)));
384  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_22", boost::cref(CHQ1_22)));
385  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_23r", boost::cref(CHQ1_23r)));
386  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_33", boost::cref(CHQ1_33)));
387  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_12i", boost::cref(CHQ1_12i)));
388  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_13i", boost::cref(CHQ1_13i)));
389  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_23i", boost::cref(CHQ1_23i)));
390  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_11", boost::cref(CHQ3_11)));
391  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_12r", boost::cref(CHQ3_12r)));
392  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_13r", boost::cref(CHQ3_13r)));
393  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_22", boost::cref(CHQ3_22)));
394  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_23r", boost::cref(CHQ3_23r)));
395  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_33", boost::cref(CHQ3_33)));
396  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_12i", boost::cref(CHQ3_12i)));
397  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_13i", boost::cref(CHQ3_13i)));
398  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_23i", boost::cref(CHQ3_23i)));
399  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_11", boost::cref(CHu_11)));
400  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_12r", boost::cref(CHu_12r)));
401  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_13r", boost::cref(CHu_13r)));
402  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_22", boost::cref(CHu_22)));
403  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_23r", boost::cref(CHu_23r)));
404  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_33", boost::cref(CHu_33)));
405  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_12i", boost::cref(CHu_12i)));
406  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_13i", boost::cref(CHu_13i)));
407  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_23i", boost::cref(CHu_23i)));
408  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_11", boost::cref(CHd_11)));
409  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_12r", boost::cref(CHd_12r)));
410  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_13r", boost::cref(CHd_13r)));
411  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_22", boost::cref(CHd_22)));
412  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_23r", boost::cref(CHd_23r)));
413  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_33", boost::cref(CHd_33)));
414  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_12i", boost::cref(CHd_12i)));
415  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_13i", boost::cref(CHd_13i)));
416  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_23i", boost::cref(CHd_23i)));
417  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_11r", boost::cref(CHud_11r)));
418  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_12r", boost::cref(CHud_12r)));
419  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_13r", boost::cref(CHud_13r)));
420  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_22r", boost::cref(CHud_22r)));
421  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_23r", boost::cref(CHud_23r)));
422  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_33r", boost::cref(CHud_33r)));
423  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_11i", boost::cref(CHud_11i)));
424  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_12i", boost::cref(CHud_12i)));
425  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_13i", boost::cref(CHud_13i)));
426  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_22i", boost::cref(CHud_22i)));
427  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_23i", boost::cref(CHud_23i)));
428  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_33i", boost::cref(CHud_33i)));
429  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11r", boost::cref(CuH_11r)));
430  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_12r", boost::cref(CuH_12r)));
431  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_13r", boost::cref(CuH_13r)));
432  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22r", boost::cref(CuH_22r)));
433  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_23r", boost::cref(CuH_23r)));
434  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33r", boost::cref(CuH_33r)));
435  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11i", boost::cref(CuH_11i)));
436  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_12i", boost::cref(CuH_12i)));
437  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_13i", boost::cref(CuH_13i)));
438  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22i", boost::cref(CuH_22i)));
439  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_23i", boost::cref(CuH_23i)));
440  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33i", boost::cref(CuH_33i)));
441  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11r", boost::cref(CdH_11r)));
442  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_12r", boost::cref(CdH_12r)));
443  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_13r", boost::cref(CdH_13r)));
444  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22r", boost::cref(CdH_22r)));
445  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_23r", boost::cref(CdH_23r)));
446  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33r", boost::cref(CdH_33r)));
447  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11i", boost::cref(CdH_11i)));
448  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_12i", boost::cref(CdH_12i)));
449  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_13i", boost::cref(CdH_13i)));
450  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22i", boost::cref(CdH_22i)));
451  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_23i", boost::cref(CdH_23i)));
452  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33i", boost::cref(CdH_33i)));
453  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_11r", boost::cref(CuG_11r)));
454  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_12r", boost::cref(CuG_12r)));
455  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_13r", boost::cref(CuG_13r)));
456  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_22r", boost::cref(CuG_22r)));
457  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_23r", boost::cref(CuG_23r)));
458  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_33r", boost::cref(CuG_33r)));
459  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_11i", boost::cref(CuG_11i)));
460  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_12i", boost::cref(CuG_12i)));
461  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_13i", boost::cref(CuG_13i)));
462  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_22i", boost::cref(CuG_22i)));
463  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_23i", boost::cref(CuG_23i)));
464  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuG_33i", boost::cref(CuG_33i)));
465  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_11r", boost::cref(CuW_11r)));
466  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_12r", boost::cref(CuW_12r)));
467  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_13r", boost::cref(CuW_13r)));
468  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_22r", boost::cref(CuW_22r)));
469  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_23r", boost::cref(CuW_23r)));
470  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_33r", boost::cref(CuW_33r)));
471  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_11i", boost::cref(CuW_11i)));
472  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_12i", boost::cref(CuW_12i)));
473  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_13i", boost::cref(CuW_13i)));
474  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_22i", boost::cref(CuW_22i)));
475  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_23i", boost::cref(CuW_23i)));
476  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuW_33i", boost::cref(CuW_33i)));
477  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_11r", boost::cref(CuB_11r)));
478  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_12r", boost::cref(CuB_12r)));
479  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_13r", boost::cref(CuB_13r)));
480  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_22r", boost::cref(CuB_22r)));
481  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_23r", boost::cref(CuB_23r)));
482  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_33r", boost::cref(CuB_33r)));
483  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_11i", boost::cref(CuB_11i)));
484  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_12i", boost::cref(CuB_12i)));
485  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_13i", boost::cref(CuB_13i)));
486  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_22i", boost::cref(CuB_22i)));
487  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_23i", boost::cref(CuB_23i)));
488  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuB_33i", boost::cref(CuB_33i)));
489  }
491  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1", boost::cref(CLQ1_1111)));
492  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3", boost::cref(CLQ3_1111)));
493  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu", boost::cref(Ceu_1111)));
494  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced", boost::cref(Ced_1111)));
495  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu", boost::cref(CLu_1111)));
496  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd", boost::cref(CLd_1111)));
497  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe", boost::cref(CQe_1111)));
498  } else {
499  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1111", boost::cref(CLQ1_1111)));
500  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1122", boost::cref(CLQ1_1122)));
501  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_2211", boost::cref(CLQ1_2211)));
502  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1221", boost::cref(CLQ1_1221)));
503  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_2112", boost::cref(CLQ1_2112)));
504  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1133", boost::cref(CLQ1_1133)));
505  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_3311", boost::cref(CLQ1_3311)));
506  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1331", boost::cref(CLQ1_1331)));
507  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_3113", boost::cref(CLQ1_3113)));
508  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1123", boost::cref(CLQ1_1123)));
509  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_2223", boost::cref(CLQ1_2223)));
510  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_3323", boost::cref(CLQ1_3323)));
511  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_1132", boost::cref(CLQ1_1132)));
512  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_2232", boost::cref(CLQ1_2232)));
513  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ1_3332", boost::cref(CLQ1_3332)));
514  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1111", boost::cref(CLQ3_1111)));
515  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1122", boost::cref(CLQ3_1122)));
516  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_2211", boost::cref(CLQ3_2211)));
517  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1221", boost::cref(CLQ3_1221)));
518  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_2112", boost::cref(CLQ3_2112)));
519  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1133", boost::cref(CLQ3_1133)));
520  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_3311", boost::cref(CLQ3_3311)));
521  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1331", boost::cref(CLQ3_1331)));
522  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_3113", boost::cref(CLQ3_3113)));
523  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1123", boost::cref(CLQ3_1123)));
524  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_2223", boost::cref(CLQ3_2223)));
525  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_3323", boost::cref(CLQ3_3323)));
526  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_1132", boost::cref(CLQ3_1132)));
527  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_2232", boost::cref(CLQ3_2232)));
528  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLQ3_3332", boost::cref(CLQ3_3332)));
529  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_1111", boost::cref(Ceu_1111)));
530  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_1122", boost::cref(Ceu_1122)));
531  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_2211", boost::cref(Ceu_2211)));
532  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_1133", boost::cref(Ceu_1133)));
533  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_2233", boost::cref(Ceu_2233)));
534  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ceu_3311", boost::cref(Ceu_3311)));
535  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_1111", boost::cref(Ced_1111)));
536  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_1122", boost::cref(Ced_1122)));
537  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_2211", boost::cref(Ced_2211)));
538  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_1133", boost::cref(Ced_1133)));
539  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_3311", boost::cref(Ced_3311)));
540  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_1123", boost::cref(Ced_1123)));
541  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_2223", boost::cref(Ced_2223)));
542  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_3323", boost::cref(Ced_3323)));
543  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_1132", boost::cref(Ced_1132)));
544  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_2232", boost::cref(Ced_2232)));
545  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Ced_3332", boost::cref(Ced_3332)));
546  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_1111", boost::cref(CLu_1111)));
547  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_1122", boost::cref(CLu_1122)));
548  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_2211", boost::cref(CLu_2211)));
549  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_1133", boost::cref(CLu_1133)));
550  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_2233", boost::cref(CLu_2233)));
551  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLu_3311", boost::cref(CLu_3311)));
552  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_1111", boost::cref(CLd_1111)));
553  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_1122", boost::cref(CLd_1122)));
554  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_2211", boost::cref(CLd_2211)));
555  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_1133", boost::cref(CLd_1133)));
556  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_3311", boost::cref(CLd_3311)));
557  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_1123", boost::cref(CLd_1123)));
558  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_2223", boost::cref(CLd_2223)));
559  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_3323", boost::cref(CLd_3323)));
560  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_1132", boost::cref(CLd_1132)));
561  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_2232", boost::cref(CLd_2232)));
562  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLd_3332", boost::cref(CLd_3332)));
563  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_1111", boost::cref(CQe_1111)));
564  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_1122", boost::cref(CQe_1122)));
565  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_2211", boost::cref(CQe_2211)));
566  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_1133", boost::cref(CQe_1133)));
567  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_3311", boost::cref(CQe_3311)));
568  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_2311", boost::cref(CQe_2311)));
569  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_2322", boost::cref(CQe_2322)));
570  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_2333", boost::cref(CQe_2333)));
571  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_3211", boost::cref(CQe_3211)));
572  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_3222", boost::cref(CQe_3222)));
573  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CQe_3233", boost::cref(CQe_3233)));
574  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLedQ_11", boost::cref(CLedQ_11)));
575  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLedQ_22", boost::cref(CLedQ_22)));
576  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CpLedQ_11", boost::cref(CpLedQ_11)));
577  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CpLedQ_22", boost::cref(CpLedQ_22)));
578  }
579  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Lambda_NP", boost::cref(Lambda_NP)));
580  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("BrHinv", boost::cref(BrHinv)));
581  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("BrHexo", boost::cref(BrHexo)));
582  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("dg1Z", boost::cref(dg1Z)));
583  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("dKappaga", boost::cref(dKappaga)));
584  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("lambZ", boost::cref(lambZ)));
585  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eggFint", boost::cref(eggFint)));
586  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eggFpar", boost::cref(eggFpar)));
587  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettHint", boost::cref(ettHint)));
588  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettHpar", boost::cref(ettHpar)));
589  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBFint", boost::cref(eVBFint)));
590  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBFpar", boost::cref(eVBFpar)));
591  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWHint", boost::cref(eWHint)));
592  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWHpar", boost::cref(eWHpar)));
593  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZHint", boost::cref(eZHint)));
594  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZHpar", boost::cref(eZHpar)));
595  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeeWBFint", boost::cref(eeeWBFint)));
596  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeeWBFpar", boost::cref(eeeWBFpar)));
597  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeeZHint", boost::cref(eeeZHint)));
598  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeeZHpar", boost::cref(eeeZHpar)));
599  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeettHint", boost::cref(eeettHint)));
600  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eeettHpar", boost::cref(eeettHpar)));
601  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHggint", boost::cref(eHggint)));
602  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHggpar", boost::cref(eHggpar)));
603  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHWWint", boost::cref(eHWWint)));
604  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHWWpar", boost::cref(eHWWpar)));
605  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHZZint", boost::cref(eHZZint)));
606  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHZZpar", boost::cref(eHZZpar)));
607  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHZgaint", boost::cref(eHZgaint)));
608  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHZgapar", boost::cref(eHZgapar)));
609  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHgagaint", boost::cref(eHgagaint)));
610  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHgagapar", boost::cref(eHgagapar)));
611  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHmumuint", boost::cref(eHmumuint)));
612  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHmumupar", boost::cref(eHmumupar)));
613  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHtautauint", boost::cref(eHtautauint)));
614  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHtautaupar", boost::cref(eHtautaupar)));
615  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHccint", boost::cref(eHccint)));
616  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHccpar", boost::cref(eHccpar)));
617  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHbbint", boost::cref(eHbbint)));
618  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eHbbpar", boost::cref(eHbbpar)));
619  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_Hbox", boost::cref(eVBF_2_Hbox)));
620  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HQ1_11", boost::cref(eVBF_2_HQ1_11)));
621  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_Hu_11", boost::cref(eVBF_2_Hu_11)));
622  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_Hd_11", boost::cref(eVBF_2_Hd_11)));
623  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HQ3_11", boost::cref(eVBF_2_HQ3_11)));
624  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HD", boost::cref(eVBF_2_HD)));
625  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HB", boost::cref(eVBF_2_HB)));
626  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HW", boost::cref(eVBF_2_HW)));
627  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HWB", boost::cref(eVBF_2_HWB)));
628  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_HG", boost::cref(eVBF_2_HG)));
629  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_DHB", boost::cref(eVBF_2_DHB)));
630  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_DHW", boost::cref(eVBF_2_DHW)));
631  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_2_DeltaGF", boost::cref(eVBF_2_DeltaGF)));
632  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_Hbox", boost::cref(eVBF_78_Hbox)));
633  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HQ1_11", boost::cref(eVBF_78_HQ1_11)));
634  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_Hu_11", boost::cref(eVBF_78_Hu_11)));
635  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_Hd_11", boost::cref(eVBF_78_Hd_11)));
636  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HQ3_11", boost::cref(eVBF_78_HQ3_11)));
637  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HD", boost::cref(eVBF_78_HD)));
638  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HB", boost::cref(eVBF_78_HB)));
639  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HW", boost::cref(eVBF_78_HW)));
640  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HWB", boost::cref(eVBF_78_HWB)));
641  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_HG", boost::cref(eVBF_78_HG)));
642  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_DHB", boost::cref(eVBF_78_DHB)));
643  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_DHW", boost::cref(eVBF_78_DHW)));
644  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_78_DeltaGF", boost::cref(eVBF_78_DeltaGF)));
645  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_Hbox", boost::cref(eVBF_1314_Hbox)));
646  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HQ1_11", boost::cref(eVBF_1314_HQ1_11)));
647  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_Hu_11", boost::cref(eVBF_1314_Hu_11)));
648  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_Hd_11", boost::cref(eVBF_1314_Hd_11)));
649  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HQ3_11", boost::cref(eVBF_1314_HQ3_11)));
650  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HD", boost::cref(eVBF_1314_HD)));
651  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HB", boost::cref(eVBF_1314_HB)));
652  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HW", boost::cref(eVBF_1314_HW)));
653  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HWB", boost::cref(eVBF_1314_HWB)));
654  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_HG", boost::cref(eVBF_1314_HG)));
655  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_DHB", boost::cref(eVBF_1314_DHB)));
656  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_DHW", boost::cref(eVBF_1314_DHW)));
657  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF_1314_DeltaGF", boost::cref(eVBF_1314_DeltaGF)));
658  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_Hbox", boost::cref(eWH_2_Hbox)));
659  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_HQ3_11", boost::cref(eWH_2_HQ3_11)));
660  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_HD", boost::cref(eWH_2_HD)));
661  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_HW", boost::cref(eWH_2_HW)));
662  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_HWB", boost::cref(eWH_2_HWB)));
663  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_DHW", boost::cref(eWH_2_DHW)));
664  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_2_DeltaGF", boost::cref(eWH_2_DeltaGF)));
665  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_Hbox", boost::cref(eWH_78_Hbox)));
666  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_HQ3_11", boost::cref(eWH_78_HQ3_11)));
667  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_HD", boost::cref(eWH_78_HD)));
668  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_HW", boost::cref(eWH_78_HW)));
669  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_HWB", boost::cref(eWH_78_HWB)));
670  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_DHW", boost::cref(eWH_78_DHW)));
671  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_78_DeltaGF", boost::cref(eWH_78_DeltaGF)));
672  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_Hbox", boost::cref(eWH_1314_Hbox)));
673  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_HQ3_11", boost::cref(eWH_1314_HQ3_11)));
674  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_HD", boost::cref(eWH_1314_HD)));
675  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_HW", boost::cref(eWH_1314_HW)));
676  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_HWB", boost::cref(eWH_1314_HWB)));
677  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_DHW", boost::cref(eWH_1314_DHW)));
678  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH_1314_DeltaGF", boost::cref(eWH_1314_DeltaGF)));
679  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_Hbox", boost::cref(eZH_2_Hbox)));
680  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HQ1_11", boost::cref(eZH_2_HQ1_11)));
681  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_Hu_11", boost::cref(eZH_2_Hu_11)));
682  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_Hd_11", boost::cref(eZH_2_Hd_11)));
683  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HQ3_11", boost::cref(eZH_2_HQ3_11)));
684  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HD", boost::cref(eZH_2_HD)));
685  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HB", boost::cref(eZH_2_HB)));
686  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HW", boost::cref(eZH_2_HW)));
687  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_HWB", boost::cref(eZH_2_HWB)));
688  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_DHB", boost::cref(eZH_2_DHB)));
689  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_DHW", boost::cref(eZH_2_DHW)));
690  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_2_DeltaGF", boost::cref(eZH_2_DeltaGF)));
691  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_Hbox", boost::cref(eZH_78_Hbox)));
692  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HQ1_11", boost::cref(eZH_78_HQ1_11)));
693  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_Hu_11", boost::cref(eZH_78_Hu_11)));
694  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_Hd_11", boost::cref(eZH_78_Hd_11)));
695  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HQ3_11", boost::cref(eZH_78_HQ3_11)));
696  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HD", boost::cref(eZH_78_HD)));
697  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HB", boost::cref(eZH_78_HB)));
698  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HW", boost::cref(eZH_78_HW)));
699  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_HWB", boost::cref(eZH_78_HWB)));
700  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_DHB", boost::cref(eZH_78_DHB)));
701  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_DHW", boost::cref(eZH_78_DHW)));
702  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_78_DeltaGF", boost::cref(eZH_78_DeltaGF)));
703  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_Hbox", boost::cref(eZH_1314_Hbox)));
704  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HQ1_11", boost::cref(eZH_1314_HQ1_11)));
705  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_Hu_11", boost::cref(eZH_1314_Hu_11)));
706  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_Hd_11", boost::cref(eZH_1314_Hd_11)));
707  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HQ3_11", boost::cref(eZH_1314_HQ3_11)));
708  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HD", boost::cref(eZH_1314_HD)));
709  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HB", boost::cref(eZH_1314_HB)));
710  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HW", boost::cref(eZH_1314_HW)));
711  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_HWB", boost::cref(eZH_1314_HWB)));
712  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_DHB", boost::cref(eZH_1314_DHB)));
713  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_DHW", boost::cref(eZH_1314_DHW)));
714  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH_1314_DeltaGF", boost::cref(eZH_1314_DeltaGF)));
715  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_2_HG", boost::cref(ettH_2_HG)));
716  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_2_G", boost::cref(ettH_2_G)));
717  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_2_uG_33r", boost::cref(ettH_2_uG_33r)));
718  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_2_DeltagHt", boost::cref(ettH_2_DeltagHt)));
719  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_78_HG", boost::cref(ettH_78_HG)));
720  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_78_G", boost::cref(ettH_78_G)));
721  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_78_uG_33r", boost::cref(ettH_78_uG_33r)));
722  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_78_DeltagHt", boost::cref(ettH_78_DeltagHt)));
723  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_1314_HG", boost::cref(ettH_1314_HG)));
724  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_1314_G", boost::cref(ettH_1314_G)));
725  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_1314_uG_33r", boost::cref(ettH_1314_uG_33r)));
726  ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH_1314_DeltagHt", boost::cref(ettH_1314_DeltagHt)));
727 
728  if (FlagLeptonUniversal) {
729  CeH_12r = 0.0;
730  CeH_13r = 0.0;
731  CeH_23r = 0.0;
732  CeH_12i = 0.0;
733  CeH_13i = 0.0;
734  CeH_23i = 0.0;
735 
736 // bsll/sbll entries only interesting (for the moment) if non-lepton universal. Set to 0 otherwise
737  CLQ1_1123 = 0.0;
738  CLQ1_2223 = 0.0;
739  CLQ1_3323 = 0.0;
740  CLQ1_1132 = 0.0;
741  CLQ1_2232 = 0.0;
742  CLQ1_3332 = 0.0;
743 
744  CLQ3_1123 = 0.0;
745  CLQ3_2223 = 0.0;
746  CLQ3_3323 = 0.0;
747  CLQ3_1132 = 0.0;
748  CLQ3_2232 = 0.0;
749  CLQ3_3332 = 0.0;
750 
751  Ced_1123 = 0.0;
752  Ced_2223 = 0.0;
753  Ced_3323 = 0.0;
754  Ced_1132 = 0.0;
755  Ced_2232 = 0.0;
756  Ced_3332 = 0.0;
757 
758  CLd_1123 = 0.0;
759  CLd_2223 = 0.0;
760  CLd_3323 = 0.0;
761  CLd_1132 = 0.0;
762  CLd_2232 = 0.0;
763  CLd_3332 = 0.0;
764 
765  CQe_2311 = 0.0;
766  CQe_2322 = 0.0;
767  CQe_2333 = 0.0;
768  CQe_3211 = 0.0;
769  CQe_3222 = 0.0;
770  CQe_3233 = 0.0;
771  }
772  if (FlagQuarkUniversal) {
773  CuH_12r = 0.0;
774  CuH_13r = 0.0;
775  CuH_23r = 0.0;
776  CuH_12i = 0.0;
777  CuH_13i = 0.0;
778  CuH_23i = 0.0;
779 
780  CdH_12r = 0.0;
781  CdH_13r = 0.0;
782  CdH_23r = 0.0;
783  CdH_12i = 0.0;
784  CdH_13i = 0.0;
785  CdH_23i = 0.0;
786  }
787 }
double Ceu_1122
Definition: NPSMEFTd6.h:3608
double CQe_2322
Definition: NPSMEFTd6.h:3631
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3552
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3542
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3429
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
double CpLedQ_22
Definition: NPSMEFTd6.h:3633
double CLL_1111
Definition: NPSMEFTd6.h:3591
gsl_integration_cquad_workspace * w_WW
Definition: NPSMEFTd6.h:3924
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3528
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
NPbase()
The default constructor.
Definition: NPbase.cpp:10
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3464
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPSMEFTd6.h:3922
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3540
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double eVBF_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3681
double eVBF_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3694
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double eVBF_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3709
double eZH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3774
double CuG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3563
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3554
double eZH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3760
double CLe_1111
Definition: NPSMEFTd6.h:3616
double eZH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3763
double eHbbpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3669
double CLQ3_1111
Definition: NPSMEFTd6.h:3599
double eHtautauint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3664
double ettH_2_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3778
double eWH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3734
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double eZH_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3738
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double eZH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3737
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3521
double CQe_2211
Definition: NPSMEFTd6.h:3629
double eZH_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3756
double CLL_1221
Definition: NPSMEFTd6.h:3592
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double eZH_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3766
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3482
double eZH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3742
double eVBF_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3706
double CLQ1_3323
Definition: NPSMEFTd6.h:3597
double CLd_1133
Definition: NPSMEFTd6.h:3625
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3590
double eZH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3748
double eWH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3721
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3494
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3508
double CuB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3587
double eVBF_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3703
double eVBF_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3707
double eWHpar
Parametric relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3643
double eZH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3768
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3544
double Ced_1111
Definition: NPSMEFTd6.h:3611
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3550
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3567
double ettHpar
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3639
double eggFpar
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3637
double eVBF_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3695
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3538
double eZH_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3759
double eHtautaupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3665
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3543
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double eVBF_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3685
double CLQ3_3323
Definition: NPSMEFTd6.h:3602
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3469
bool FlagUnivOfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and ...
Definition: NPSMEFTd6.h:3907
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3463
double CLL_1331
Definition: NPSMEFTd6.h:3593
double CH
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3443
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3515
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3549
double CLQ3_2223
Definition: NPSMEFTd6.h:3602
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3461
double Cee_1133
Definition: NPSMEFTd6.h:3606
double Ced_2232
Definition: NPSMEFTd6.h:3615
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3579
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
double CLQ3_2112
Definition: NPSMEFTd6.h:3600
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3640
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double eVBF_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3687
double Ceu_2233
Definition: NPSMEFTd6.h:3610
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CuW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3571
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3511
double eWH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3714
double eZH_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3753
double eVBF_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3672
double eVBF_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3674
double eVBF_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3671
double CuW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3577
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3654
double eVBF_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3673
double CuB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3586
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3481
double Ced_1132
Definition: NPSMEFTd6.h:3615
double CLu_1133
Definition: NPSMEFTd6.h:3621
double CLQ1_2112
Definition: NPSMEFTd6.h:3595
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3477
double eZH_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3743
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3506
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3510
double CHWHB_gagaorth
The combination of dimension-6 operator coefficients .
Definition: NPSMEFTd6.h:3437
double ettH_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3776
double CLQ3_1122
Definition: NPSMEFTd6.h:3600
Matching< NPSMEFTd6Matching, NPSMEFTd6 > NPSMEFTd6M
Definition: NPSMEFTd6.h:3427
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3555
double eHmumuint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3662
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3649
double eZH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3773
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3650
double eVBF_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3683
double CLQ3_2232
Definition: NPSMEFTd6.h:3603
double eVBF_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3686
double eZH_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3764
double eVBF_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3700
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3535
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3585
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3547
double eVBF_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3689
double dg1Z
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3796
double CLL_1133
Definition: NPSMEFTd6.h:3593
double eHgagaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3660
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3529
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3641
double eZH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3758
double ettH_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3781
double eVBF_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3701
double CLd_1123
Definition: NPSMEFTd6.h:3626
double CuB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3589
T & getObj()
Definition: Matching.h:16
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3512
double eWH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3718
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3493
double eZH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3747
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3468
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3514
double Ced_3323
Definition: NPSMEFTd6.h:3614
double eWH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3723
double eWH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3716
double eVBF_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3696
double CLQ3_1123
Definition: NPSMEFTd6.h:3602
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3798
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3566
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3452
double eHggpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3653
double eWH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3724
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:3904
double eVBF_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3691
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3655
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3473
A class for the matching in the Standard Model.
double CLQ1_1133
Definition: NPSMEFTd6.h:3596
double Ced_1123
Definition: NPSMEFTd6.h:3614
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3553
double CLe_3311
Definition: NPSMEFTd6.h:3618
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3519
double ettH_1314_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3787
double CLQ1_1123
Definition: NPSMEFTd6.h:3597
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double C2B
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3431
double CLd_2223
Definition: NPSMEFTd6.h:3626
double CLQ1_3311
Definition: NPSMEFTd6.h:3596
double eHZgaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3658
double eHbbint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3668
double eWH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3725
Matching< StandardModelMatching, StandardModel > SMM
An object of type Matching.
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3558
double CLedQ_22
Definition: NPSMEFTd6.h:3633
double ettH_2_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3777
double CLQ1_2211
Definition: NPSMEFTd6.h:3595
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CLd_1111
Definition: NPSMEFTd6.h:3623
double eVBF_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3676
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3518
double CLQ1_1111
Definition: NPSMEFTd6.h:3594
double Ced_1133
Definition: NPSMEFTd6.h:3613
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3570
double eWH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3722
double eHZgapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3659
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double C2W
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3432
double Ceu_1133
Definition: NPSMEFTd6.h:3609
double CuW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3568
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3576
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3504
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3509
double eZH_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3739
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3491
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3525
double eWH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3726
double Ceu_3311
Definition: NPSMEFTd6.h:3609
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3466
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3520
double eZH_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3740
double CLQ3_1221
Definition: NPSMEFTd6.h:3600
double eVBF_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3693
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3651
double eZH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3745
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3541
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3648
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3513
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3457
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3460
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3496
double CLd_1132
Definition: NPSMEFTd6.h:3627
double CLQ1_1331
Definition: NPSMEFTd6.h:3596
void setObj(T &obji)
Definition: Matching.h:17
double eZH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3741
double dKappaga
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3797
double CQe_3222
Definition: NPSMEFTd6.h:3632
double CLu_3311
Definition: NPSMEFTd6.h:3621
double CLd_1122
Definition: NPSMEFTd6.h:3624
double CLe_1122
Definition: NPSMEFTd6.h:3617
double CLu_2233
Definition: NPSMEFTd6.h:3622
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients...
Definition: NPSMEFTd6.h:3906
double CLQ3_1133
Definition: NPSMEFTd6.h:3601
double CLedQ_11
Definition: NPSMEFTd6.h:3633
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
double CQe_3233
Definition: NPSMEFTd6.h:3632
double Ceu_2211
Definition: NPSMEFTd6.h:3608
double eWH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3733
double ettH_1314_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3788
double CLQ3_3113
Definition: NPSMEFTd6.h:3601
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3472
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double eVBF_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3704
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3430
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3516
double eZH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3744
double CuB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3581
double CQe_2333
Definition: NPSMEFTd6.h:3631
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3551
double ettH_78_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3784
double CLQ3_1331
Definition: NPSMEFTd6.h:3601
double CuG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3562
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3531
double CQe_1122
Definition: NPSMEFTd6.h:3629
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3445
double Ceu_1111
Definition: NPSMEFTd6.h:3607
bool FlagHiggsSM
A boolean flag that is true if including dependence on small variations of the SM parameters (depende...
Definition: NPSMEFTd6.h:3908
double eHggint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3652
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3523
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3486
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3446
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3495
double Ced_3332
Definition: NPSMEFTd6.h:3615
double CuB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3583
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPSMEFTd6.h:3916
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3450
double ettH_78_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3783
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3459
double CLe_2211
Definition: NPSMEFTd6.h:3617
double eWH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3732
double eVBF_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3711
double eWH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3730
double CpLedQ_11
Definition: NPSMEFTd6.h:3633
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3470
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3546
bool FlagPartialQFU
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd fa...
Definition: NPSMEFTd6.h:3905
double Ced_2223
Definition: NPSMEFTd6.h:3614
double CLQ1_3113
Definition: NPSMEFTd6.h:3596
double CLu_2211
Definition: NPSMEFTd6.h:3620
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3582
double CuG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3565
double CLQ3_1132
Definition: NPSMEFTd6.h:3603
double ettH_2_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3779
double CLL_1122
Definition: NPSMEFTd6.h:3592
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3502
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3507
double CLd_2211
Definition: NPSMEFTd6.h:3624
double CQe_3211
Definition: NPSMEFTd6.h:3632
double eHccint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3666
double CLQ1_2232
Definition: NPSMEFTd6.h:3598
double CLQ1_1122
Definition: NPSMEFTd6.h:3595
double eHgagapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3661
double CuW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3569
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3479
double CLd_3323
Definition: NPSMEFTd6.h:3626
double ettH_78_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3782
double eZH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3761
double eVBF_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3692
double eZH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3754
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
double eVBF_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3702
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794
double CuG_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3559
double CLd_3332
Definition: NPSMEFTd6.h:3627
double CLQ1_2223
Definition: NPSMEFTd6.h:3597
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3527
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3448
double ettH_1314_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3789
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double eWH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3713
double CLQ3_3311
Definition: NPSMEFTd6.h:3601
double CuW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3575
double eZHint
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3644
double eZH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3771
double eZH_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3769
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3505
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
double eZH_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3772
double eVBF_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3699
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3588
double eWHint
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3642
double eWH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3729
double CLd_3311
Definition: NPSMEFTd6.h:3625
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3517
double CLQ3_2211
Definition: NPSMEFTd6.h:3600
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3478
double eVBF_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3688
double eZH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3750
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3578
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:3909
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double eWH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3717
bool FlagLoopH3d6Quad
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables...
Definition: NPSMEFTd6.h:3910
double CLQ1_1132
Definition: NPSMEFTd6.h:3598
double eVBF_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3677
double CuG_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3556
double eVBF_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3682
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3573
double CLQ3_3332
Definition: NPSMEFTd6.h:3603
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3500
double CQe_1111
Definition: NPSMEFTd6.h:3628
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3561
double Ced_2211
Definition: NPSMEFTd6.h:3612
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double eZH_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3765
double CuW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3574
double ettH_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3786
double CLQ1_1221
Definition: NPSMEFTd6.h:3595
double Ced_3311
Definition: NPSMEFTd6.h:3613
double CLd_2232
Definition: NPSMEFTd6.h:3627
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double eHccpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3667
double CLu_1122
Definition: NPSMEFTd6.h:3620
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3499
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double eWH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3715
double ettHint
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3638
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3539
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eZH_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3752
double eVBF_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3697
double eVBF_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3678
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:3793
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3484
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3533
double eWH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3727
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3497
void setModelLinearized(bool linearized=true)
Definition: Model.h:222
double eHmumupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3663
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3490
double eZH_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3751
double eVBF_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3679
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:3634
double CuG_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3557
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double CLu_1111
Definition: NPSMEFTd6.h:3619
double eZH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3755
double CuB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3580
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3526
double eVBF_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3680
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3537
double Cee_1122
Definition: NPSMEFTd6.h:3605
double CHWHB_gaga
The combination of dimension-6 operator coefficients entering in : .
Definition: NPSMEFTd6.h:3436
double eZHpar
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3645
double eWH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3735
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
std::map< std::string, boost::reference_wrapper< const double > > ModelParamMap
Definition: Model.h:241
double eggFint
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3636
double CQe_3311
Definition: NPSMEFTd6.h:3630
double eZH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3770
double eWH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3719
double eVBF_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3705
double eZH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3767
double eWH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3731
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3487
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3475
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3451
double Ced_1122
Definition: NPSMEFTd6.h:3612
double eVBF_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3690
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3530
double eVBF_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3675
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3564
double Cee_1111
Definition: NPSMEFTd6.h:3604
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3454
double eZH_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3746
double CLe_1133
Definition: NPSMEFTd6.h:3618
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3455
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3545
double CQe_1133
Definition: NPSMEFTd6.h:3630
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3488
double CLQ1_3332
Definition: NPSMEFTd6.h:3598
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3532
double eZH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3757
double CQe_2311
Definition: NPSMEFTd6.h:3631
double eVBF_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3710
double eVBF_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3708
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

Member Function Documentation

◆ AH_f()

gslpp::complex NPSMEFTd6::AH_f ( const double  tau) const

Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)

Parameters
[in]

Definition at line 3029 of file NPSMEFTd6.cpp.

3030 {
3031  return (2.0 * tau * (1.0 + (1.0 - tau) * f_triangle(tau)));
3032 }
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:2985

◆ AH_W()

gslpp::complex NPSMEFTd6::AH_W ( const double  tau) const

W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.

\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)

Parameters
[in]

Definition at line 3034 of file NPSMEFTd6.cpp.

3035 {
3036  return -( 2.0 + 3.0 * tau + 3.0 * tau * (2.0 - tau) * f_triangle(tau) );
3037 }
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:2985

◆ AHZga_f()

gslpp::complex NPSMEFTd6::AHZga_f ( const double  tau,
const double  lambda 
) const

Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3039 of file NPSMEFTd6.cpp.

3040 {
3041  return I_triangle_1(tau,lambda) - I_triangle_2(tau,lambda);
3042 }
gslpp::complex I_triangle_2(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3020
double lambda
The CKM parameter in the Wolfenstein parameterization.
gslpp::complex I_triangle_1(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3009

◆ AHZga_W()

gslpp::complex NPSMEFTd6::AHZga_W ( const double  tau,
const double  lambda 
) const

W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3044 of file NPSMEFTd6.cpp.

3045 {
3046  gslpp::complex tmp;
3047 
3048  double tan2w = trueSM.sW2() / trueSM.cW2();
3049 
3050  tmp = 4.0 * (3.0 - tan2w ) * I_triangle_2(tau,lambda);
3051 
3052  tmp = tmp + ((1.0 +2.0 / tau)* tan2w - (5.0 + 2.0/tau)) * I_triangle_1(tau,lambda);
3053 
3054  return sqrt(trueSM.cW2()) * tmp;
3055 }
gslpp::complex I_triangle_2(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3020
StandardModel trueSM
Definition: NPbase.h:1902
virtual double cW2(const double Mw_i) const
The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as ...
double lambda
The CKM parameter in the Wolfenstein parameterization.
virtual double sW2(const double Mw_i) const
The square of the sine of the weak mixing angle in the on-shell scheme, denoted as ...
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
gslpp::complex I_triangle_1(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3009
complex sqrt(const complex &z)

◆ AuxObs_NP1()

double NPSMEFTd6::AuxObs_NP1 ( ) const
virtual

Auxiliary observable AuxObs_NP1 (See code for details.)

Returns
AuxObs_NP1

Reimplemented from NPbase.

Definition at line 12901 of file NPSMEFTd6.cpp.

12902 {
12903  // To be used for some temporary observable
12904 
12905  // WY analysis at 13 TeV for HL-LHC 3/ab
12906  double Wpar, Ypar, Wpar2, Ypar2;
12907  double Chi2NC13, Chi2CC13, Chi2Tot;
12908 
12909  Wpar = 10000.0 * obliqueW();
12910  Ypar = 10000.0 * obliqueY();
12911 
12912  Wpar2 = Wpar*Wpar;
12913  Ypar2 = Ypar*Ypar;
12914 
12915  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
12916 
12917  Chi2NC13 = 0.032772034538390675 * Wpar2*Wpar2 + 2.815243944990361 * Ypar2 - 0.36522061776278516 * Ypar2*Ypar
12918  + 0.017375258924241194 * Ypar2*Ypar2 + Wpar2*Wpar * (-0.7059117582389635 + 0.006816297425306027 * Ypar)
12919  + Wpar * Ypar * (7.988302197022343 + Ypar * (-0.5450119819316416 + 0.0050292149953719766 * Ypar))
12920  + Wpar2 * (5.68581760491364 + Ypar * (-0.5794111075840261 + 0.048026245835369625 * Ypar));
12921 
12922  Chi2Tot = Chi2CC13 + Chi2NC13;
12923 
12924  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
12925  return sqrt(Chi2Tot);
12926 }
virtual double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2376
virtual double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2381
complex sqrt(const complex &z)

◆ AuxObs_NP2()

double NPSMEFTd6::AuxObs_NP2 ( ) const
virtual

Auxiliary observable AuxObs_NP2 (See code for details.)

Returns
AuxObs_NP2

Reimplemented from NPbase.

Definition at line 12928 of file NPSMEFTd6.cpp.

12929 {
12930  // To be used for some temporary observable
12931 
12932  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
12933  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 5% systematics (corr and uncorr)
12934  double Wpar, Ypar, Wpar2, Ypar2;
12935  double Chi2NC27, Chi2CC13, Chi2Tot;
12936 
12937  Wpar = 10000.0 * obliqueW();
12938  Ypar = 10000.0 * obliqueY();
12939 
12940  Wpar2 = Wpar*Wpar;
12941  Ypar2 = Ypar*Ypar;
12942 
12943  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
12944 
12945  Chi2NC27 = 21.139285368181907 * Wpar2*Wpar2 + Wpar2*Wpar * (-89.16828370317616 + 7.182929295852857 * Ypar)
12946  + Wpar * Ypar * (208.8092257396059 + Ypar * (-81.00102926445666 + 6.203591096144735 * Ypar))
12947  + Ypar2 * (81.01075991905888 + Ypar * (-58.822719932531164 + 14.670206406369107 * Ypar))
12948  + Wpar2 * (136.70787790194357 + Ypar * (-86.48485007990255 + 35.67671393730628 * Ypar));
12949 
12950  Chi2Tot = Chi2CC13 + Chi2NC27;
12951 
12952  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
12953  return sqrt(Chi2Tot);
12954 }
virtual double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2376
virtual double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2381
complex sqrt(const complex &z)

◆ AuxObs_NP3()

double NPSMEFTd6::AuxObs_NP3 ( ) const
virtual

Auxiliary observable AuxObs_NP3 (See code for details.)

Returns
AuxObs_NP3

Reimplemented from NPbase.

Definition at line 12956 of file NPSMEFTd6.cpp.

12957 {
12958  // To be used for some temporary observable
12959 
12960  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
12961  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 1% systematics (corr and uncorr)
12962  double Wpar, Ypar, Wpar2, Ypar2;
12963  double Chi2NC27, Chi2CC13, Chi2Tot;
12964 
12965  Wpar = 10000.0 * obliqueW();
12966  Ypar = 10000.0 * obliqueY();
12967 
12968  Wpar2 = Wpar*Wpar;
12969  Ypar2 = Ypar*Ypar;
12970 
12971  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
12972 
12973  Chi2NC27 = 25.148424251427552 * Wpar2*Wpar2 + Wpar2*Wpar * (-105.31753344410277 + 8.01723084630248 * Ypar)
12974  + Wpar * Ypar * (253.11721255992683 + Ypar * (-93.18990615818014 + 6.8250043104055816 * Ypar))
12975  + Ypar2 * (97.52107126224298 + Ypar * (-67.961770347904945 + 16.80046890875678 * Ypar))
12976  + Wpar2 * (166.84179829911304 + Ypar * (-100.88118582829852 + 41.55424691040131 * Ypar));
12977 
12978  Chi2Tot = Chi2CC13 + Chi2NC27;
12979 
12980  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
12981  return sqrt(Chi2Tot);
12982 }
virtual double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2376
virtual double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2381
complex sqrt(const complex &z)

◆ AuxObs_NP4()

double NPSMEFTd6::AuxObs_NP4 ( ) const
virtual

Auxiliary observable AuxObs_NP4 (See code for details.)

Returns
AuxObs_NP4

Reimplemented from NPbase.

Definition at line 12984 of file NPSMEFTd6.cpp.

12985 {
12986  // To be used for some temporary observable
12987  return 0.0;
12988 }

◆ AuxObs_NP5()

double NPSMEFTd6::AuxObs_NP5 ( ) const
virtual

Auxiliary observable AuxObs_NP5 (See code for details.)

Returns
AuxObs_NP5

Reimplemented from NPbase.

Definition at line 12990 of file NPSMEFTd6.cpp.

12991 {
12992  // To be used for some temporary observable
12993  return 0.0;
12994 }

◆ AuxObs_NP6()

double NPSMEFTd6::AuxObs_NP6 ( ) const
virtual

Auxiliary observable AuxObs_NP6 (See code for details.)

Returns
AuxObs_NP6

Reimplemented from NPbase.

Definition at line 12996 of file NPSMEFTd6.cpp.

12997 {
12998  // To be used for some temporary observable
12999 
13000  // HL-LHC DiHiggs invariant mass distribution: 14 TeV 3/ab
13001 
13002  double Chi2Tot;
13003 
13004 // NP in decays
13005  double dGH2,dGgaga,dGbb, dBRTot;
13006 
13007 // Contributions from the different bins
13008  double Bin1,Bin2,Bin3,Bin4,Bin5,Bin6;
13009  double LLBin1, LLBin2, LLBin3, LLBin4, LLBin5, LLBin6;
13010 
13011 // Higgs basis parameters
13012  double dcZHB,cZboxHB,cZZHB,cZgaHB,cgagaHB,cggHB;
13013  double dytHB,dybHB,dytauHB;
13014  double dKlambda;
13015 
13016  dcZHB = deltacZ_HB();
13017  cZboxHB = cZBox_HB();
13018  cZZHB = cZZ_HB();
13019 
13020 // In the paper it seems they use diff. norm but in the chi 2.nb
13021 // they translate into that convention, so I assume their calculation
13022 // is directly in the HB for the following 3 couplings
13023  cZgaHB = cZga_HB();
13024  cgagaHB = cgaga_HB();
13025  cggHB = cgg_HB();
13026 
13027  dytHB = deltayt_HB();
13028  dybHB = deltayb_HB();
13029  dytauHB = deltaytau_HB();
13030 
13031  dKlambda = deltaG_hhhRatio();
13032 
13033 // Corrections to the different Higgs widths
13034  dGH2 = 1. + 0.010512791990056657 * cZboxHB
13035  - 0.003819752423722165 * cZZHB + 0.0016024991450954641 * cZgaHB
13036  - 0.0005968238492400916 * (2.8975474398595105 * cZboxHB
13037  + 1.8975474398595107 * cZZHB - cZgaHB - 0.3426378481886507 * cgagaHB)
13038  + 0.0990750425382019 * (1.4487737199297552 * cZboxHB + 0.44877371992975534 * cZZHB
13039  - 0.2365019764475461 * cZgaHB - 0.08103452830235015 * cgagaHB)
13040  - 0.0330404571742506 * (cZZHB + 0.4730039528950922 * cZgaHB + 0.055933184863595636 * cgagaHB)
13041  - 0.00033171593951211893 * cgagaHB + 0.48287726036165796 * dcZHB
13042  + 1.1541846695471276 * dybHB + 0.12642022723635785 * dytauHB
13043  + 0.1704272683629381 * (0. + 118.68284969347252 * cggHB
13044  - 0.031082871395970327 * dybHB + 1.034601498835783 * dytHB)
13045  + 0.004560729716754681 * (0. - 12.079950077697095 * cgagaHB
13046  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
13047  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB)
13048  + 0.003080492878860618 * (0. - 17.021015025105033 * cZgaHB
13049  + 1.0557935963831278 * dcZHB + 0.0006235357344154619 * dybHB
13050  - 0.05644023795399054 * dytHB + 0.000023105836447458856 * dytauHB);
13051 
13052  dGH2 = dGH2 * dGH2;
13053 
13054  dGgaga = 1.0 + 2.0 * (0. - 12.079950077697095 * cgagaHB
13055  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
13056  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB);
13057 
13058  dGbb = 1.0 + 2.0 * dybHB;
13059 
13060  dBRTot = dGbb * dGgaga / dGH2;
13061 
13062  // Bin 1
13063  Bin1 = 0.17*(1.0 + 3.9863794294589585 * cggHB
13064  + 21.333394807321064 * cggHB*cggHB + 3.9527789724382836 * dcZHB
13065  + 0.5566823785534646 * cggHB*dcZHB + 9.077153576669469 * dcZHB*dcZHB
13066  - 7.713285621354339 * dytHB + 6.573887966178747 * cggHB*dytHB
13067  - 45.88983201032187 * dcZHB*dytHB + 62.42156375416841 * dytHB*dytHB
13068  + 4.257555672380181 * cggHB*dytHB*dytHB + 4.620310477256665 * dcZHB*dytHB*dytHB
13069  - 9.403185493195476 * dytHB*dytHB*dytHB + 1.1563473213070041 * dytHB*dytHB*dytHB*dytHB
13070  - 0.14505129596051047 * dKlambda - 0.1418831193390564 * cggHB*dKlambda
13071  + 1.3502693869386464 * cggHB*cggHB*dKlambda - 0.6675315048183816 * dcZHB*dKlambda
13072  - 0.002999558395846163 * cggHB*dcZHB*dKlambda
13073  + 1.5448485758806263 * dytHB * dKlambda
13074  - 0.005002986050963205 * cggHB*dytHB*dKlambda
13075  - 0.6675315048183816 * dcZHB*dytHB * dKlambda
13076  + 1.5222565251876392 * dytHB*dytHB * dKlambda
13077  + 0.1278814581005547 * cggHB*dytHB*dytHB * dKlambda
13078  - 0.1676433466534976 * dytHB*dytHB*dytHB * dKlambda
13079  + 0.011296025346493552 * dKlambda*dKlambda
13080  + 0.0014116654816114353 * cggHB*dKlambda*dKlambda
13081  + 0.022260157195710357 * cggHB*cggHB*dKlambda*dKlambda
13082  + 0.022592050692987104 * dytHB * dKlambda*dKlambda
13083  + 0.0014116654816114353 * cggHB*dytHB*dKlambda*dKlambda
13084  + 0.011296025346493552 * dytHB*dytHB * dKlambda*dKlambda);
13085 
13086  Bin1 = 0.67944 + Bin1 * dBRTot;
13087 
13088  // Exclude points with negative values of BinX
13089  if ( Bin1 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13090 
13091  // Delta chi2 = -2*LL for the bin
13092  // Add an abs in the denominator of the log,
13093  // even if events with negative BinX are not supposed to reach here.
13094  LLBin1 = 2.0 * (Bin1 - 0.84944 + 0.84944 * log( 0.84944 / fabs(Bin1) ) );
13095 
13096  // Bin 2
13097  Bin2 = 0.33*(1.0 + 1.8019627645351037 * cggHB
13098  + 7.953163597932105 * cggHB*cggHB + 3.735123481549394 * dcZHB
13099  - 2.654186900737259 * cggHB*dcZHB + 6.403420811368324 * dcZHB*dcZHB
13100  - 6.991501690350679 * dytHB + 11.425848100026737 * cggHB*dytHB
13101  - 30.219763494155394 * dcZHB*dytHB + 39.692409895713936 * dytHB*dytHB
13102  + 1.661324633279857 * cggHB*dytHB*dytHB + 4.46563789250516 * dcZHB*dytHB*dytHB
13103  - 8.710706509282613 * dytHB*dytHB*dytHB + 1.2361692069676826 * dytHB*dytHB*dytHB*dytHB
13104  - 0.21386875429750188 * dKlambda + 0.2363972133088796 * cggHB*dKlambda
13105  + 0.8549707073528667 * cggHB*cggHB*dKlambda - 0.7305144109557659 * dcZHB*dKlambda
13106  - 0.14136602060890807 * cggHB*dcZHB*dKlambda + 1.50533606463443 * dytHB * dKlambda
13107  + 0.747017712869579 * cggHB*dytHB*dKlambda - 0.7305144109557659 * dcZHB*dytHB * dKlambda
13108  + 1.4607351592940678 * dytHB*dytHB * dKlambda
13109  + 0.08652243773397514 * cggHB*dytHB*dytHB * dKlambda
13110  - 0.25846965963786395 * dytHB*dytHB*dytHB * dKlambda
13111  + 0.022300452670181038 * dKlambda*dKlambda + 0.009236644319657653 * cggHB*dKlambda*dKlambda
13112  + 0.023125582948149842 * cggHB*cggHB*dKlambda*dKlambda
13113  + 0.044600905340362075 * dytHB * dKlambda*dKlambda
13114  + 0.009236644319657653 * cggHB*dytHB*dKlambda*dKlambda
13115  + 0.022300452670181038 * dytHB*dytHB * dKlambda*dKlambda) ;
13116 
13117  Bin2 = 1.4312 + Bin2 * dBRTot;
13118 
13119  // Exclude points with negative values of BinX
13120  if ( Bin2 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13121 
13122  // Delta chi2 = -2*LL for the bin
13123  // Add an abs in the denominator of the log,
13124  // even if events with negative BinX are not supposed to reach here.
13125  LLBin2 = 2.0 * (Bin2 - 1.7612 + 1.7612 * log( 1.7612 / fabs(Bin2) ) );
13126 
13127  // Bin 3
13128  Bin3 = 0.99*(1.0 + 0.6707152151845268 * cggHB
13129  + 4.113022405261353 * cggHB*cggHB + 3.4241906309399726 * dcZHB
13130  - 2.9926046286644703 * cggHB*dcZHB + 4.72026565086762 * dcZHB*dcZHB
13131  - 5.98522416048399 * dytHB + 10.012680455917307 * cggHB*dytHB
13132  - 20.69102310585157 * dcZHB*dytHB + 26.4871108999121 * dytHB*dytHB
13133  + 0.36415135473936855 * cggHB*dytHB*dytHB
13134  + 4.206380168414172 * dcZHB*dytHB*dytHB - 7.688318821918381 * dytHB*dytHB*dytHB
13135  + 1.3217369754941033 * dytHB*dytHB*dytHB*dytHB - 0.2873477323359291 * dKlambda
13136  + 0.35631144357921507 * cggHB*dKlambda
13137  + 0.6197019283831009 * cggHB*cggHB*dKlambda
13138  - 0.7821895374741993 * dcZHB*dKlambda
13139  - 0.23172596419155064 * cggHB*dcZHB*dKlambda
13140  + 1.415746929098462 * dytHB * dKlambda
13141  + 1.0816714186441074 * cggHB*dytHB*dKlambda
13142  - 0.7821895374741993 * dcZHB*dytHB * dKlambda
13143  + 1.3469684427821131 * dytHB*dytHB * dKlambda
13144  + 0.030182082490240562 * cggHB*dytHB*dytHB * dKlambda
13145  - 0.35612621865227795 * dytHB*dytHB*dytHB * dKlambda
13146  + 0.03438924315817444 * dKlambda*dKlambda
13147  + 0.019565500643816278 * cggHB*dKlambda*dKlambda
13148  + 0.02382411268034237 * cggHB*cggHB*dKlambda*dKlambda
13149  + 0.06877848631634888 * dytHB * dKlambda*dKlambda
13150  + 0.019565500643816278 * cggHB*dytHB*dKlambda*dKlambda
13151  + 0.03438924315817444 * dytHB*dytHB * dKlambda*dKlambda);
13152 
13153  Bin3 = 1.9764 + Bin3 * dBRTot;
13154 
13155  // Exclude points with negative values of BinX
13156  if ( Bin3 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13157 
13158  // Delta chi2 = -2*LL for the bin
13159  // Add an abs in the denominator of the log,
13160  // even if events with negative BinX are not supposed to reach here.
13161  LLBin3 = 2.0 * (Bin3 - 2.9664 + 2.9664 * log( 2.9664 / fabs(Bin3) ) );
13162 
13163  // Bin 4
13164  Bin4 = 2.86*(1.0 - 0.27406342847042814 * cggHB
13165  + 1.9597360046161074 * cggHB*cggHB + 3.0113078755334115 * dcZHB
13166  - 2.776019265892887 * cggHB*dcZHB + 3.1917709639679823 * dcZHB*dcZHB
13167  - 4.6362529563760955 * dytHB + 7.377234185667426 * cggHB*dytHB
13168  - 12.294598143269557 * dcZHB*dytHB + 15.407456380301479 * dytHB*dytHB
13169  - 0.6767601835408067 * cggHB*dytHB*dytHB
13170  + 3.844719765004924 * dcZHB*dytHB*dytHB
13171  - 6.227970053277897 * dytHB*dytHB*dytHB + 1.4542592857563688 * dytHB*dytHB*dytHB*dytHB
13172  - 0.39767067022413716 * dKlambda + 0.3661464075997459 * cggHB*dKlambda
13173  + 0.4464409042746693 * cggHB*cggHB*dKlambda
13174  - 0.8334118894715125 * dcZHB*dKlambda
13175  - 0.3263197431214281 * cggHB*dcZHB*dKlambda
13176  + 1.1940464266776625 * dytHB * dKlambda
13177  + 1.2643073873631234 * cggHB*dytHB*dKlambda
13178  - 0.8334118894715125 * dcZHB*dytHB * dKlambda
13179  + 1.0808691956131988 * dytHB*dytHB * dKlambda
13180  - 0.0807982496009068 * cggHB*dytHB*dytHB * dKlambda
13181  - 0.5108479012886007 * dytHB*dytHB*dytHB * dKlambda
13182  + 0.05658861553223176 * dKlambda*dKlambda
13183  + 0.04424790213027415 * cggHB*dKlambda*dKlambda
13184  + 0.02585578262020257 * cggHB*cggHB*dKlambda*dKlambda
13185  + 0.11317723106446352 * dytHB * dKlambda*dKlambda
13186  + 0.04424790213027415 * cggHB*dytHB*dKlambda*dKlambda
13187  + 0.05658861553223176 * dytHB*dytHB * dKlambda*dKlambda);
13188 
13189  Bin4 = 5.167 + Bin4 * dBRTot;
13190 
13191  // Exclude points with negative values of BinX
13192  if ( Bin4 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13193 
13194  // Delta chi2 = -2*LL for the bin
13195  // Add an abs in the denominator of the log,
13196  // even if events with negative BinX are not supposed to reach here.
13197  LLBin4 = 2.0 * (Bin4 - 8.027 + 8.027 * log( 8.027 / fabs(Bin4) ) );
13198 
13199  // Bin 5
13200  Bin5 = 6.34* (1.0 - 1.094329254675176 * cggHB
13201  + 1.0393648302909912 * cggHB*cggHB + 2.6000916816530903 * dcZHB
13202  - 2.4448264513323226 * cggHB*dcZHB + 2.073935963891534 * dcZHB*dcZHB
13203  - 3.192332240205929 * dytHB + 4.5914586198385 * cggHB*dytHB
13204  - 6.2871857258718595 * dcZHB*dytHB + 8.134770266934664 * dytHB*dytHB
13205  - 1.648691479483292 * cggHB*dytHB*dytHB + 3.5563383758242524 * dcZHB*dytHB*dytHB
13206  - 4.615570013047001 * dytHB*dytHB*dytHB + 1.7227511548362076 * dytHB*dytHB*dytHB*dytHB
13207  - 0.6079428047533413 * dKlambda + 0.33825211279194234 * cggHB*dKlambda
13208  + 0.3879052211526028 * cggHB*cggHB*dKlambda - 0.956246694171162 * dcZHB*dKlambda
13209  - 0.4572431444456198 * cggHB*dcZHB*dKlambda + 0.8152949680877302 * dytHB * dKlambda
13210  + 1.3814632626914451 * cggHB*dytHB*dKlambda
13211  - 0.956246694171162 * dcZHB*dytHB * dKlambda + 0.5856782679219981 * dytHB*dytHB * dKlambda
13212  - 0.3285182834373566 * cggHB*dytHB*dytHB * dKlambda
13213  - 0.8375595049190734 * dytHB*dytHB*dytHB * dKlambda + 0.11480835008286604 * dKlambda*dKlambda
13214  + 0.11240817142118299 * cggHB*dKlambda*dKlambda + 0.03688252014841459 * cggHB*cggHB*dKlambda*dKlambda
13215  + 0.22961670016573207 * dytHB * dKlambda*dKlambda
13216  + 0.11240817142118299 * cggHB*dytHB*dKlambda*dKlambda
13217  + 0.11480835008286604 * dytHB*dytHB * dKlambda*dKlambda);
13218 
13219  Bin5 = 15.93 + Bin5 * dBRTot;
13220 
13221  // Exclude points with negative values of BinX
13222  if ( Bin5 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13223 
13224  // Delta chi2 = -2*LL for the bin
13225  // Add an abs in the denominator of the log,
13226  // even if events with negative BinX are not supposed to reach here.
13227  LLBin5 = 2.0 * (Bin5 - 22.27 + 22.27 * log( 22.27 / fabs(Bin5) ) );
13228 
13229  // Bin 6
13230  Bin6 = 2.14*(1.0 - 2.007855065799201 * cggHB + 1.1994575008850934 * cggHB*cggHB
13231  + 2.5987763498382352 * dcZHB - 2.908713303420072 * cggHB*dcZHB
13232  + 1.804645897901265 * dcZHB*dcZHB - 2.806900956988577 * dytHB
13233  + 3.5621616844486415 * cggHB*dytHB - 4.250685020965587 * dcZHB*dytHB
13234  + 5.7468374752045515 * dytHB*dytHB - 3.1561231600123736 * cggHB*dytHB*dytHB
13235  + 3.9784140166037667 * dcZHB*dytHB*dytHB - 4.4303353405513395 * dytHB*dytHB*dytHB
13236  + 2.257739308366916 * dytHB*dytHB*dytHB*dytHB - 0.9894280925261291 * dKlambda
13237  + 0.589956279744333 * cggHB*dKlambda + 0.6687315933211253 * cggHB*cggHB*dKlambda
13238  - 1.3796376667655315 * dcZHB*dKlambda - 0.8069993678124955 * cggHB*dcZHB*dKlambda
13239  + 0.6340062910366335 * dytHB * dKlambda + 2.127573647123277 * cggHB*dytHB*dKlambda
13240  - 1.3796376667655315 * dcZHB*dytHB * dKlambda + 0.09738385935505989 * dytHB*dytHB * dKlambda
13241  - 0.8833807360585424 * cggHB*dytHB*dytHB * dKlambda - 1.5260505242077027 * dytHB*dytHB*dytHB * dKlambda
13242  + 0.2683112158407868 * dKlambda*dKlambda + 0.32506892158970235 * cggHB*dKlambda*dKlambda
13243  + 0.09418943796384227 * cggHB*cggHB*dKlambda*dKlambda + 0.5366224316815736 * dytHB * dKlambda*dKlambda
13244  + 0.32506892158970235 * cggHB*dytHB*dKlambda*dKlambda
13245  + 0.2683112158407868 * dytHB*dytHB * dKlambda*dKlambda);
13246 
13247  Bin6 = 12.01 + Bin6 * dBRTot;
13248 
13249  // Exclude points with negative values of BinX
13250  if ( Bin6 < 0 ) return std::numeric_limits<double>::quiet_NaN();
13251 
13252  // Delta chi2 = -2*LL for the bin
13253  // Add an abs in the denominator of the log,
13254  // even if events with negative BinX are not supposed to reach here.
13255  LLBin6 = 2.0 * (Bin6 - 14.15 + 14.15 * log( 14.15 / fabs(Bin6) ) );
13256 
13257  // The total contributions to the log-likelihood/chi-square
13258  Chi2Tot = LLBin1 + LLBin2 + LLBin3 + LLBin4 + LLBin5 + LLBin6;
13259 
13260  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
13261  return sqrt(Chi2Tot);
13262 }
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.)
virtual double cZga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double cgaga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double deltaytau_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double deltayt_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.)
virtual double deltayb_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.)
virtual double cgg_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double cZZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
complex log(const complex &z)
virtual double cZBox_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual double deltacZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.)
complex sqrt(const complex &z)

◆ Br_H_exo()

double NPSMEFTd6::Br_H_exo ( ) const
virtual

The branching ratio of the of the Higgs into exotic particles.

Returns
Br \((H\to exotic)\)

Reimplemented from NPbase.

Definition at line 11730 of file NPSMEFTd6.cpp.

11731 {
11732  if (BrHexo < 0) return std::numeric_limits<double>::quiet_NaN();
11733 
11734  return BrHexo;
11735 }
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794

◆ Br_H_inv()

double NPSMEFTd6::Br_H_inv ( ) const
virtual

The branching ratio of the of the Higgs into invisible particles.

Returns
Br \((H\to invisible)\)

Reimplemented from NPbase.

Definition at line 11737 of file NPSMEFTd6.cpp.

11738 {
11739 // Contributions from both modifications in H->ZZ->4v and the extra invisible decays
11740  double BR4v;
11741 
11742  BR4v = BrHZZ4vRatio()*(trueSM.computeBrHtoZZinv());
11743 
11744 // BR4v positivity is already checked inside BrHZZ4vRatio()
11745 // and will be nan if negative. Check here BrHinv, to make sure both are positive
11746  if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
11747 
11748  return BR4v + BrHinv;
11749 }
virtual double BrHZZ4vRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9580
StandardModel trueSM
Definition: NPbase.h:1902
double computeBrHtoZZinv() const
The Br in the Standard Model.
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:3793

◆ BrHbbRatio()

double NPSMEFTd6::BrHbbRatio ( ) const
virtual

The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.

Returns
Br \((H\to b\bar{b})\)/Br \((H\to b\bar{b})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9905 of file NPSMEFTd6.cpp.

9906 {
9907  double Br = 1.0;
9908  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9909 
9910  dGHiR1= deltaGammaHbbRatio1();
9911 
9912  Br += dGHiR1 - dGammaHTotR1;
9913 
9914  if (FlagQuadraticTerms) {
9915 
9916  dGHiR2= deltaGammaHbbRatio2();
9917 
9918  //Add contributions that are quadratic in the effective coefficients
9919  Br += - dGHiR1 * dGammaHTotR1
9920  + dGHiR2 - dGammaHTotR2
9921  + pow(dGammaHTotR1,2.0);
9922  }
9923 
9924  GHiR += dGHiR1 + dGHiR2;
9925  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9926 
9927  return Br;
9928 
9929 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ BrHccRatio()

double NPSMEFTd6::BrHccRatio ( ) const
virtual

The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.

Returns
Br \((H\to c\bar{c})\)/Br \((H\to c\bar{c})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9879 of file NPSMEFTd6.cpp.

9880 {
9881  double Br = 1.0;
9882  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9883 
9884  dGHiR1= deltaGammaHccRatio1();
9885 
9886  Br += dGHiR1 - dGammaHTotR1;
9887 
9888  if (FlagQuadraticTerms) {
9889 
9890  dGHiR2= deltaGammaHccRatio2();
9891 
9892  //Add contributions that are quadratic in the effective coefficients
9893  Br += - dGHiR1 * dGammaHTotR1
9894  + dGHiR2 - dGammaHTotR2
9895  + pow(dGammaHTotR1,2.0);
9896  }
9897 
9898  GHiR += dGHiR1 + dGHiR2;
9899  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9900 
9901  return Br;
9902 
9903 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHgagaRatio()

double NPSMEFTd6::BrHgagaRatio ( ) const
virtual

The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to \gamma\gamma)\)/Br \((H\to \gamma\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9801 of file NPSMEFTd6.cpp.

9802 {
9803  double Br = 1.0;
9804  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9805 
9806  dGHiR1= deltaGammaHgagaRatio1();
9807 
9808  Br += dGHiR1 - dGammaHTotR1;
9809 
9810  if (FlagQuadraticTerms) {
9811 
9812  dGHiR2= deltaGammaHgagaRatio2();
9813 
9814  //Add contributions that are quadratic in the effective coefficients
9815  Br += - dGHiR1 * dGammaHTotR1
9816  + dGHiR2 - dGammaHTotR2
9817  + pow(dGammaHTotR1,2.0);
9818  }
9819 
9820  GHiR += dGHiR1 + dGHiR2;
9821  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9822 
9823  return Br;
9824 
9825 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ BrHggRatio()

double NPSMEFTd6::BrHggRatio ( ) const
virtual

The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.

Returns
Br \((H\to gg)\)/Br \((H\to gg)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9241 of file NPSMEFTd6.cpp.

9242 {
9243  double Br = 1.0;
9244  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9245 
9246  dGHiR1= deltaGammaHggRatio1();
9247 
9248  Br += dGHiR1 - dGammaHTotR1;
9249 
9250  if (FlagQuadraticTerms) {
9251 
9252  dGHiR2= deltaGammaHggRatio2();
9253 
9254  //Add contributions that are quadratic in the effective coefficients
9255  Br += - dGHiR1 * dGammaHTotR1
9256  + dGHiR2 - dGammaHTotR2
9257  + pow(dGammaHTotR1,2.0);
9258  }
9259 
9260  GHiR += dGHiR1 + dGHiR2;
9261  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9262 
9263  return Br;
9264 
9265 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ BrHmumuRatio()

double NPSMEFTd6::BrHmumuRatio ( ) const
virtual

The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \mu^+\mu^-)\)/Br \((H\to \mu^+\mu^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9827 of file NPSMEFTd6.cpp.

9828 {
9829  double Br = 1.0;
9830  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9831 
9832  dGHiR1= deltaGammaHmumuRatio1();
9833 
9834  Br += dGHiR1 - dGammaHTotR1;
9835 
9836  if (FlagQuadraticTerms) {
9837 
9838  dGHiR2= deltaGammaHmumuRatio2();
9839 
9840  //Add contributions that are quadratic in the effective coefficients
9841  Br += - dGHiR1 * dGammaHTotR1
9842  + dGHiR2 - dGammaHTotR2
9843  + pow(dGammaHTotR1,2.0);
9844  }
9845 
9846  GHiR += dGHiR1 + dGHiR2;
9847  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9848 
9849  return Br;
9850 
9851 }
complex pow(const complex &z1, const complex &z2)
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHtautauRatio()

double NPSMEFTd6::BrHtautauRatio ( ) const
virtual

The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \tau^+\tau^-)\)/Br \((H\to \tau^+\tau^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9853 of file NPSMEFTd6.cpp.

9854 {
9855  double Br = 1.0;
9856  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9857 
9858  dGHiR1= deltaGammaHtautauRatio1();
9859 
9860  Br += dGHiR1 - dGammaHTotR1;
9861 
9862  if (FlagQuadraticTerms) {
9863 
9864  dGHiR2= deltaGammaHtautauRatio2();
9865 
9866  //Add contributions that are quadratic in the effective coefficients
9867  Br += - dGHiR1 * dGammaHTotR1
9868  + dGHiR2 - dGammaHTotR2
9869  + pow(dGammaHTotR1,2.0);
9870  }
9871 
9872  GHiR += dGHiR1 + dGHiR2;
9873  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9874 
9875  return Br;
9876 
9877 }
complex pow(const complex &z1, const complex &z2)
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHtoinvRatio()

double NPSMEFTd6::BrHtoinvRatio ( ) const
virtual

The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.

Returns
Br \((H\to invisible)\)/Br \((H\to ZZ \to invisible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 11800 of file NPSMEFTd6.cpp.

11801 {
11802  return (Br_H_inv()/(trueSM.computeBrHtoZZinv()));
11803 }
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Br_H_inv() const
The branching ratio of the of the Higgs into invisible particles.
double computeBrHtoZZinv() const
The Br in the Standard Model.

◆ BrHvisRatio()

double NPSMEFTd6::BrHvisRatio ( ) const
virtual

The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.

Returns
Br \((H\to visible)\)/Br \((H\to visible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 11752 of file NPSMEFTd6.cpp.

11753 {
11754  double Br = 1.0;
11755  double dvis1 = 0.0, dvis2 = 0.0, delta2SM;
11756  double GHvisR = 1.0;
11757 
11758 // Sum over decays of visible SM and exotic modes
11768  + BrHexo);
11769 
11770  Br += dvis1 - dGammaHTotR1;
11771 
11772  if (FlagQuadraticTerms) {
11773 
11774 // Sum over decays of visible SM and exotic modes
11775  delta2SM = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
11784 
11785  dvis2 = delta2SM + (BrHexo)*(BrHexo + delta2SM);
11786 
11787  //Add contributions that are quadratic in the effective coefficients
11788  Br += - dvis1 * dGammaHTotR1
11789  + dvis2 - dGammaHTotR2
11790  + pow(dGammaHTotR1,2.0);
11791  }
11792 
11793  GHvisR += dvis1 + dvis2;
11794  if ((Br < 0) || (GHvisR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
11795 
11796  return Br;
11797 }
double computeBrHtocc() const
The Br in the Standard Model.
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double computeBrHtoZga() const
The Br in the Standard Model.
StandardModel trueSM
Definition: NPbase.h:1902
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtoWW() const
The Br in the Standard Model.
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtomumu() const
The Br in the Standard Model.
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double computeBrHtoZZ() const
The Br in the Standard Model.
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtotautau() const
The Br in the Standard Model.
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794
double computeBrHtogg() const
The Br in the Standard Model.
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double computeBrHtogaga() const
The Br in the Standard Model.
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtobb() const
The Br in the Standard Model.
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ BrHWffRatio()

double NPSMEFTd6::BrHWffRatio ( ) const
virtual

The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to W f f)\)/Br \((H\to W f f)_{\mathrm{SM}}\)

Definition at line 9374 of file NPSMEFTd6.cpp.

9375 {
9376  double Br = 1.0;
9377  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9378 
9379  dGHiR1= deltaGammaHWffRatio1();
9380 
9381  Br += dGHiR1 - dGammaHTotR1;
9382 
9383  if (FlagQuadraticTerms) {
9384 
9385  dGHiR2= deltaGammaHWffRatio2();
9386 
9387  //Add contributions that are quadratic in the effective coefficients
9388  Br += - dGHiR1 * dGammaHTotR1
9389  + dGHiR2 - dGammaHTotR2
9390  + pow(dGammaHTotR1,2.0);
9391  }
9392 
9393  GHiR += dGHiR1 + dGHiR2;
9394  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9395 
9396  return Br;
9397 }
double deltaGammaHWffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ BrHWjjRatio()

double NPSMEFTd6::BrHWjjRatio ( ) const
virtual

The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.

Returns
Br \((H\to W j j)\)/Br \((H\to W j j)_{\mathrm{SM}}\)

Definition at line 9324 of file NPSMEFTd6.cpp.

9325 {
9326  double Br = 1.0;
9327  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9328 
9329  dGHiR1= deltaGammaHWjjRatio1();
9330 
9331  Br += dGHiR1 - dGammaHTotR1;
9332 
9333  if (FlagQuadraticTerms) {
9334 
9335  dGHiR2= deltaGammaHWjjRatio2();
9336 
9337  //Add contributions that are quadratic in the effective coefficients
9338  Br += - dGHiR1 * dGammaHTotR1
9339  + dGHiR2 - dGammaHTotR2
9340  + pow(dGammaHTotR1,2.0);
9341  }
9342 
9343  GHiR += dGHiR1 + dGHiR2;
9344  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9345 
9346  return Br;
9347 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHWjjRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWjjRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ BrHWlvRatio()

double NPSMEFTd6::BrHWlvRatio ( ) const
virtual

The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Wl\nu)\)/Br \((H\to Wl\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9274 of file NPSMEFTd6.cpp.

9275 {
9276  double Br = 1.0;
9277  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9278 
9279  dGHiR1= deltaGammaHWlvRatio1();
9280 
9281  Br += dGHiR1 - dGammaHTotR1;
9282 
9283  if (FlagQuadraticTerms) {
9284 
9285  dGHiR2= deltaGammaHWlvRatio2();
9286 
9287  //Add contributions that are quadratic in the effective coefficients
9288  Br += - dGHiR1 * dGammaHTotR1
9289  + dGHiR2 - dGammaHTotR2
9290  + pow(dGammaHTotR1,2.0);
9291  }
9292 
9293  GHiR += dGHiR1 + dGHiR2;
9294  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9295 
9296  return Br;
9297 }
double deltaGammaHWlvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWlvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...

◆ BrHWW2l2vRatio()

double NPSMEFTd6::BrHWW2l2vRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to l\nu l\nu)\)/Br \((H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9299 of file NPSMEFTd6.cpp.

9300 {
9301  double Br = 1.0;
9302  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9303 
9304  dGHiR1= deltaGammaHWW2l2vRatio1();
9305 
9306  Br += dGHiR1 - dGammaHTotR1;
9307 
9308  if (FlagQuadraticTerms) {
9309 
9310  dGHiR2= deltaGammaHWW2l2vRatio2();
9311 
9312  //Add contributions that are quadratic in the effective coefficients
9313  Br += - dGHiR1 * dGammaHTotR1
9314  + dGHiR2 - dGammaHTotR2
9315  + pow(dGammaHTotR1,2.0);
9316  }
9317 
9318  GHiR += dGHiR1 + dGHiR2;
9319  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9320 
9321  return Br;
9322 }
double deltaGammaHWW2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHWW2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHWW4fRatio()

double NPSMEFTd6::BrHWW4fRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4f)\)/Br \((H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 9400 of file NPSMEFTd6.cpp.

9401 {
9402  double Br = 1.0;
9403  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9404 
9405  dGHiR1= deltaGammaHWW4fRatio1();
9406 
9407  Br += dGHiR1 - dGammaHTotR1;
9408 
9409  if (FlagQuadraticTerms) {
9410 
9411  dGHiR2= deltaGammaHWW4fRatio2();
9412 
9413  //Add contributions that are quadratic in the effective coefficients
9414  Br += - dGHiR1 * dGammaHTotR1
9415  + dGHiR2 - dGammaHTotR2
9416  + pow(dGammaHTotR1,2.0);
9417  }
9418 
9419  GHiR += dGHiR1 + dGHiR2;
9420  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9421 
9422  return Br;
9423 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHWW4jRatio()

double NPSMEFTd6::BrHWW4jRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4j)\)/Br \((H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 9349 of file NPSMEFTd6.cpp.

9350 {
9351  double Br = 1.0;
9352  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9353 
9354  dGHiR1= deltaGammaHWW4jRatio1();
9355 
9356  Br += dGHiR1 - dGammaHTotR1;
9357 
9358  if (FlagQuadraticTerms) {
9359 
9360  dGHiR2= deltaGammaHWW4jRatio2();
9361 
9362  //Add contributions that are quadratic in the effective coefficients
9363  Br += - dGHiR1 * dGammaHTotR1
9364  + dGHiR2 - dGammaHTotR2
9365  + pow(dGammaHTotR1,2.0);
9366  }
9367 
9368  GHiR += dGHiR1 + dGHiR2;
9369  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9370 
9371  return Br;
9372 }
double deltaGammaHWW4jRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHWW4jRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHWWRatio()

double NPSMEFTd6::BrHWWRatio ( ) const
virtual

The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW)\)/Br \((H\to WW)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9267 of file NPSMEFTd6.cpp.

9268 {
9269 
9270  return BrHWW4fRatio();
9271 
9272 }
virtual double BrHWW4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model...
Definition: NPSMEFTd6.cpp:9400

◆ BrHZddRatio()

double NPSMEFTd6::BrHZddRatio ( ) const
virtual

The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z d d)\)/Br \((H\to Z d d)_{\mathrm{SM}}\)

Definition at line 9645 of file NPSMEFTd6.cpp.

9646 {
9647  double Br = 1.0;
9648  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9649 
9650  dGHiR1= deltaGammaHZddRatio1();
9651 
9652  Br += dGHiR1 - dGammaHTotR1;
9653 
9654  if (FlagQuadraticTerms) {
9655 
9656  dGHiR2= deltaGammaHZddRatio2();
9657 
9658  //Add contributions that are quadratic in the effective coefficients
9659  Br += - dGHiR1 * dGammaHTotR1
9660  + dGHiR2 - dGammaHTotR2
9661  + pow(dGammaHTotR1,2.0);
9662  }
9663 
9664  GHiR += dGHiR1 + dGHiR2;
9665  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9666 
9667  return Br;
9668 }
complex pow(const complex &z1, const complex &z2)
double deltaGammaHZddRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHZddRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...

◆ BrHZffRatio()

double NPSMEFTd6::BrHZffRatio ( ) const
virtual

The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to Zff)\)/Br \((H\to Zff)_{\mathrm{SM}}\)

Definition at line 9688 of file NPSMEFTd6.cpp.

9689 {
9690  double Br = 1.0;
9691  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9692 
9693  dGHiR1= deltaGammaHZffRatio1();
9694 
9695  Br += dGHiR1 - dGammaHTotR1;
9696 
9697  if (FlagQuadraticTerms) {
9698 
9699  dGHiR2= deltaGammaHZffRatio2();
9700 
9701  //Add contributions that are quadratic in the effective coefficients
9702  Br += - dGHiR1 * dGammaHTotR1
9703  + dGHiR2 - dGammaHTotR2
9704  + pow(dGammaHTotR1,2.0);
9705  }
9706 
9707  GHiR += dGHiR1 + dGHiR2;
9708  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9709 
9710  return Br;
9711 }
double deltaGammaHZffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
double deltaGammaHZffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZgaeeRatio()

double NPSMEFTd6::BrHZgaeeRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ee\gamma)\)/Br \((H\to Z\gamma\to ee\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9779 of file NPSMEFTd6.cpp.

9780 {
9781  double deltaBRratio;
9782 
9783  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON]) / (trueSM.GammaZ(leptons[ELECTRON]));
9784 
9785  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
9786 
9787  return ( BrHZgaRatio() + deltaBRratio );
9788 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle leptons[6]
An array of Particle objects for the leptons.

◆ BrHZgallRatio()

double NPSMEFTd6::BrHZgallRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ll\gamma)\)/Br \((H\to Z\gamma\to ll\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9764 of file NPSMEFTd6.cpp.

9765 {
9766  double deltaBRratio;
9767 
9768  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
9769  + deltaGamma_Zf(leptons[MU]);
9770 
9771  deltaBRratio = deltaBRratio /
9773 
9774  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
9775 
9776  return ( BrHZgaRatio() + deltaBRratio );
9777 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: QCD.h:605

◆ BrHZgamumuRatio()

double NPSMEFTd6::BrHZgamumuRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to \mu\mu\gamma)\)/Br \((H\to Z\gamma\to \mu\mu\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9790 of file NPSMEFTd6.cpp.

9791 {
9792  double deltaBRratio;
9793 
9794  deltaBRratio = deltaGamma_Zf(leptons[MU])/(trueSM.GammaZ(leptons[MU]));
9795 
9796  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
9797 
9798  return ( BrHZgaRatio() + deltaBRratio );
9799 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: QCD.h:605

◆ BrHZgaRatio()

double NPSMEFTd6::BrHZgaRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma)\)/Br \((H\to Z\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9738 of file NPSMEFTd6.cpp.

9739 {
9740  double Br = 1.0;
9741  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9742 
9743  dGHiR1= deltaGammaHZgaRatio1();
9744 
9745  Br += dGHiR1 - dGammaHTotR1;
9746 
9747  if (FlagQuadraticTerms) {
9748 
9749  dGHiR2= deltaGammaHZgaRatio2();
9750 
9751  //Add contributions that are quadratic in the effective coefficients
9752  Br += - dGHiR1 * dGammaHTotR1
9753  + dGHiR2 - dGammaHTotR2
9754  + pow(dGammaHTotR1,2.0);
9755  }
9756 
9757  GHiR += dGHiR1 + dGHiR2;
9758  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9759 
9760  return Br;
9761 
9762 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZllRatio()

double NPSMEFTd6::BrHZllRatio ( ) const
virtual

The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Zll)\)/Br \((H\to Zll)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9430 of file NPSMEFTd6.cpp.

9431 {
9432  double Br = 1.0;
9433  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9434 
9435  dGHiR1= deltaGammaHZllRatio1();
9436 
9437  Br += dGHiR1 - dGammaHTotR1;
9438 
9439  if (FlagQuadraticTerms) {
9440 
9441  dGHiR2= deltaGammaHZllRatio2();
9442 
9443  //Add contributions that are quadratic in the effective coefficients
9444  Br += - dGHiR1 * dGammaHTotR1
9445  + dGHiR2 - dGammaHTotR2
9446  + pow(dGammaHTotR1,2.0);
9447  }
9448 
9449  GHiR += dGHiR1 + dGHiR2;
9450  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9451 
9452  return Br;
9453 }
double deltaGammaHZllRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHZllRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZuuRatio()

double NPSMEFTd6::BrHZuuRatio ( ) const
virtual

The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z u u)\)/Br \((H\to Z u u)_{\mathrm{SM}}\)

Definition at line 9605 of file NPSMEFTd6.cpp.

9606 {
9607  double Br = 1.0;
9608  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9609 
9610  dGHiR1= deltaGammaHZuuRatio1();
9611 
9612  Br += dGHiR1 - dGammaHTotR1;
9613 
9614  if (FlagQuadraticTerms) {
9615 
9616  dGHiR2= deltaGammaHZuuRatio2();
9617 
9618  //Add contributions that are quadratic in the effective coefficients
9619  Br += - dGHiR1 * dGammaHTotR1
9620  + dGHiR2 - dGammaHTotR2
9621  + pow(dGammaHTotR1,2.0);
9622  }
9623 
9624  GHiR += dGHiR1 + dGHiR2;
9625  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9626 
9627  return Br;
9628 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHZuuRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZuuRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZvvRatio()

double NPSMEFTd6::BrHZvvRatio ( ) const
virtual

The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\nu\nu)\)/Br \((H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 9555 of file NPSMEFTd6.cpp.

9556 {
9557  double Br = 1.0;
9558  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9559 
9560  dGHiR1= deltaGammaHZvvRatio1();
9561 
9562  Br += dGHiR1 - dGammaHTotR1;
9563 
9564  if (FlagQuadraticTerms) {
9565 
9566  dGHiR2= deltaGammaHZvvRatio2();
9567 
9568  //Add contributions that are quadratic in the effective coefficients
9569  Br += - dGHiR1 * dGammaHTotR1
9570  + dGHiR2 - dGammaHTotR2
9571  + pow(dGammaHTotR1,2.0);
9572  }
9573 
9574  GHiR += dGHiR1 + dGHiR2;
9575  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9576 
9577  return Br;
9578 }
double deltaGammaHZvvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZvvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZ2e2muRatio()

double NPSMEFTd6::BrHZZ2e2muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 2e 2\mu)\)/Br \((H\to ZZ* \to 2e 2\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9505 of file NPSMEFTd6.cpp.

9506 {
9507  double Br = 1.0;
9508  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9509 
9510  dGHiR1= deltaGammaHZZ2e2muRatio1();
9511 
9512  Br += dGHiR1 - dGammaHTotR1;
9513 
9514  if (FlagQuadraticTerms) {
9515 
9516  dGHiR2= deltaGammaHZZ2e2muRatio2();
9517 
9518  //Add contributions that are quadratic in the effective coefficients
9519  Br += - dGHiR1 * dGammaHTotR1
9520  + dGHiR2 - dGammaHTotR2
9521  + pow(dGammaHTotR1,2.0);
9522  }
9523 
9524  GHiR += dGHiR1 + dGHiR2;
9525  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9526 
9527  return Br;
9528 }
complex pow(const complex &z1, const complex &z2)
double deltaGammaHZZ2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZ4dRatio()

double NPSMEFTd6::BrHZZ4dRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 d)\)/Br \((H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 9670 of file NPSMEFTd6.cpp.

9671 {
9672  double deltaBRratio;
9673 
9674  deltaBRratio = deltaGamma_Zf(quarks[DOWN])
9677 
9678  deltaBRratio = deltaBRratio /
9679  ( trueSM.GammaZ(quarks[DOWN])
9681  + trueSM.GammaZ(quarks[BOTTOM]) );
9682 
9683  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
9684 
9685  return ( BrHZddRatio() + deltaBRratio );
9686 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Definition: QCD.h:616
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual double BrHZddRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9645

◆ BrHZZ4eRatio()

double NPSMEFTd6::BrHZZ4eRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4e)\)/Br \((H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9480 of file NPSMEFTd6.cpp.

9481 {
9482  double Br = 1.0;
9483  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9484 
9485  dGHiR1= deltaGammaHZZ4eRatio1();
9486 
9487  Br += dGHiR1 - dGammaHTotR1;
9488 
9489  if (FlagQuadraticTerms) {
9490 
9491  dGHiR2= deltaGammaHZZ4eRatio2();
9492 
9493  //Add contributions that are quadratic in the effective coefficients
9494  Br += - dGHiR1 * dGammaHTotR1
9495  + dGHiR2 - dGammaHTotR2
9496  + pow(dGammaHTotR1,2.0);
9497  }
9498 
9499  GHiR += dGHiR1 + dGHiR2;
9500  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9501 
9502  return Br;
9503 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZ4fRatio()

double NPSMEFTd6::BrHZZ4fRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4f)\)/Br \((H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 9713 of file NPSMEFTd6.cpp.

9714 {
9715  double Br = 1.0;
9716  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9717 
9718  dGHiR1= deltaGammaHZZ4fRatio1();
9719 
9720  Br += dGHiR1 - dGammaHTotR1;
9721 
9722  if (FlagQuadraticTerms) {
9723 
9724  dGHiR2= deltaGammaHZZ4fRatio2();
9725 
9726  //Add contributions that are quadratic in the effective coefficients
9727  Br += - dGHiR1 * dGammaHTotR1
9728  + dGHiR2 - dGammaHTotR2
9729  + pow(dGammaHTotR1,2.0);
9730  }
9731 
9732  GHiR += dGHiR1 + dGHiR2;
9733  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9734 
9735  return Br;
9736 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ BrHZZ4lRatio()

double NPSMEFTd6::BrHZZ4lRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4l)\)/Br \((H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9455 of file NPSMEFTd6.cpp.

9456 {
9457  double Br = 1.0;
9458  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9459 
9460  dGHiR1= deltaGammaHZZ4lRatio1();
9461 
9462  Br += dGHiR1 - dGammaHTotR1;
9463 
9464  if (FlagQuadraticTerms) {
9465 
9466  dGHiR2= deltaGammaHZZ4lRatio2();
9467 
9468  //Add contributions that are quadratic in the effective coefficients
9469  Br += - dGHiR1 * dGammaHTotR1
9470  + dGHiR2 - dGammaHTotR2
9471  + pow(dGammaHTotR1,2.0);
9472  }
9473 
9474  GHiR += dGHiR1 + dGHiR2;
9475  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9476 
9477  return Br;
9478 }
double deltaGammaHZZ4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZ4muRatio()

double NPSMEFTd6::BrHZZ4muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\mu)\)/Br \((H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9530 of file NPSMEFTd6.cpp.

9531 {
9532  double Br = 1.0;
9533  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9534 
9535  dGHiR1= deltaGammaHZZ4muRatio1();
9536 
9537  Br += dGHiR1 - dGammaHTotR1;
9538 
9539  if (FlagQuadraticTerms) {
9540 
9541  dGHiR2= deltaGammaHZZ4muRatio2();
9542 
9543  //Add contributions that are quadratic in the effective coefficients
9544  Br += - dGHiR1 * dGammaHTotR1
9545  + dGHiR2 - dGammaHTotR2
9546  + pow(dGammaHTotR1,2.0);
9547  }
9548 
9549  GHiR += dGHiR1 + dGHiR2;
9550  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9551 
9552  return Br;
9553 }
complex pow(const complex &z1, const complex &z2)
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZ4uRatio()

double NPSMEFTd6::BrHZZ4uRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 u)\)/Br \((H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 9630 of file NPSMEFTd6.cpp.

9631 {
9632  double deltaBRratio;
9633 
9634  deltaBRratio = deltaGamma_Zf(quarks[UP])
9636 
9637  deltaBRratio = deltaBRratio /
9639 
9640  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
9641 
9642  return ( BrHZuuRatio() + deltaBRratio );
9643 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
virtual double BrHZuuRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9605
StandardModel trueSM
Definition: NPbase.h:1902
Definition: QCD.h:615
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222

◆ BrHZZ4vRatio()

double NPSMEFTd6::BrHZZ4vRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\nu)\)/Br \((H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 9580 of file NPSMEFTd6.cpp.

9581 {
9582  double Br = 1.0;
9583  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
9584 
9585  dGHiR1= deltaGammaHZZ4vRatio1();
9586 
9587  Br += dGHiR1 - dGammaHTotR1;
9588 
9589  if (FlagQuadraticTerms) {
9590 
9591  dGHiR2= deltaGammaHZZ4vRatio2();
9592 
9593  //Add contributions that are quadratic in the effective coefficients
9594  Br += - dGHiR1 * dGammaHTotR1
9595  + dGHiR2 - dGammaHTotR2
9596  + pow(dGammaHTotR1,2.0);
9597  }
9598 
9599  GHiR += dGHiR1 + dGHiR2;
9600  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
9601 
9602  return Br;
9603 }
complex pow(const complex &z1, const complex &z2)
double deltaGammaHZZ4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double deltaGammaHZZ4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ BrHZZRatio()

double NPSMEFTd6::BrHZZRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ)\)/Br \((H\to ZZ)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9425 of file NPSMEFTd6.cpp.

9426 {
9427  return BrHZZ4fRatio();
9428 }
virtual double BrHZZ4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model...
Definition: NPSMEFTd6.cpp:9713

◆ CfB_diag()

gslpp::complex NPSMEFTd6::CfB_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fB})_{ff} \(\)

Definition at line 2327 of file NPSMEFTd6.cpp.

2328 {
2329  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2330  return 0.0;
2331  else if (f.is("ELECTRON"))
2332  return 0.0;
2333  else if (f.is("MU"))
2334  return 0.0;
2335  else if (f.is("TAU"))
2336  return 0.0;
2337  else if (f.is("UP"))
2338  return gslpp::complex(CuB_11r, CuB_11i, false);
2339  else if (f.is("CHARM"))
2340  return gslpp::complex(CuB_22r, CuB_22i, false);
2341  else if (f.is("TOP"))
2342  return gslpp::complex(CuB_33r, CuB_33i, false);
2343  else if (f.is("DOWN"))
2344  return 0.0;
2345  else if (f.is("STRANGE"))
2346  return 0.0;
2347  else if (f.is("BOTTOM"))
2348  return 0.0;
2349  else
2350  throw std::runtime_error("NPSMEFTd6::CfB_diag(): wrong argument");
2351 }
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3590
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3579
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3585
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3582
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3588
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ CfG_diag()

gslpp::complex NPSMEFTd6::CfG_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fG})_{ff} \(\)

Definition at line 2275 of file NPSMEFTd6.cpp.

2276 {
2277  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2278  return 0.0;
2279  else if (f.is("ELECTRON"))
2280  return 0.0;
2281  else if (f.is("MU"))
2282  return 0.0;
2283  else if (f.is("TAU"))
2284  return 0.0;
2285  else if (f.is("UP"))
2286  return gslpp::complex(CuG_11r, CuG_11i, false);
2287  else if (f.is("CHARM"))
2288  return gslpp::complex(CuG_22r, CuG_22i, false);
2289  else if (f.is("TOP"))
2290  return gslpp::complex(CuG_33r, CuG_33i, false);
2291  else if (f.is("DOWN"))
2292  return 0.0;
2293  else if (f.is("STRANGE"))
2294  return 0.0;
2295  else if (f.is("BOTTOM"))
2296  return 0.0;
2297  else
2298  throw std::runtime_error("NPSMEFTd6::CfG_diag(): wrong argument");
2299 }
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3555
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3566
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3558
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3561
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3564

◆ CfH_diag()

gslpp::complex NPSMEFTd6::CfH_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fH})_{ff} \(\)

Definition at line 2249 of file NPSMEFTd6.cpp.

2250 {
2251  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2252  return 0.0;
2253  else if (f.is("ELECTRON"))
2254  return gslpp::complex(CeH_11r, CeH_11i, false);
2255  else if (f.is("MU"))
2256  return gslpp::complex(CeH_22r, CeH_22i, false);
2257  else if (f.is("TAU"))
2258  return gslpp::complex(CeH_33r, CeH_33i, false);
2259  else if (f.is("UP"))
2260  return gslpp::complex(CuH_11r, CuH_11i, false);
2261  else if (f.is("CHARM"))
2262  return gslpp::complex(CuH_22r, CuH_22i, false);
2263  else if (f.is("TOP"))
2264  return gslpp::complex(CuH_33r, CuH_33i, false);
2265  else if (f.is("DOWN"))
2266  return gslpp::complex(CdH_11r, CdH_11i, false);
2267  else if (f.is("STRANGE"))
2268  return gslpp::complex(CdH_22r, CdH_22i, false);
2269  else if (f.is("BOTTOM"))
2270  return gslpp::complex(CdH_33r, CdH_33i, false);
2271  else
2272  throw std::runtime_error("NPSMEFTd6::CfH_diag(): wrong argument");
2273 }
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3552
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3542
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3528
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3540
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3554
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3543
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3549
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3519
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3525
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3531
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3546
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3537
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3530

◆ CfW_diag()

gslpp::complex NPSMEFTd6::CfW_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fW})_{ff} \(\)

Definition at line 2301 of file NPSMEFTd6.cpp.

2302 {
2303  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2304  return 0.0;
2305  else if (f.is("ELECTRON"))
2306  return 0.0;
2307  else if (f.is("MU"))
2308  return 0.0;
2309  else if (f.is("TAU"))
2310  return 0.0;
2311  else if (f.is("UP"))
2312  return gslpp::complex(CuW_11r, CuW_11i, false);
2313  else if (f.is("CHARM"))
2314  return gslpp::complex(CuW_22r, CuW_22i, false);
2315  else if (f.is("TOP"))
2316  return gslpp::complex(CuW_33r, CuW_33i, false);
2317  else if (f.is("DOWN"))
2318  return 0.0;
2319  else if (f.is("STRANGE"))
2320  return 0.0;
2321  else if (f.is("BOTTOM"))
2322  return 0.0;
2323  else
2324  throw std::runtime_error("NPSMEFTd6::CfW_diag(): wrong argument");
2325 }
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3567
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3570
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3576
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3578
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3573
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35

◆ cgaga_HB()

double NPSMEFTd6::cgaga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12870 of file NPSMEFTd6.cpp.

12871 {
12872  double ciHB;
12873 
12875 
12876  return ciHB;
12877 }
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804

◆ cgg_HB()

double NPSMEFTd6::cgg_HB ( ) const
virtual

The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{gg}\)

Reimplemented from NPbase.

Definition at line 12880 of file NPSMEFTd6.cpp.

12881 {
12882  double ciHB;
12883 
12884  ciHB = (1.0/(M_PI * AlsMz))*CHG*v2_over_LambdaNP2;
12885 
12886  return ciHB;
12887 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double AlsMz
The strong coupling constant at the Z-boson mass, .
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ CheckParameters()

bool NPSMEFTd6::CheckParameters ( const std::map< std::string, double > &  DPars)
virtual

A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.

Parameters
[in]DParsa map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2087 of file NPSMEFTd6.cpp.

2088 {
2090  if (FlagRotateCHWCHB) {
2091  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2092  if (DPars.find(NPSMEFTd6VarsRot_LFU_QFU[i]) == DPars.end()) {
2093  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2094  << NPSMEFTd6VarsRot_LFU_QFU[i] << std::endl;
2095  return false;
2096  }
2097  }
2098  } else {
2099  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2100  if (DPars.find(NPSMEFTd6Vars_LFU_QFU[i]) == DPars.end()) {
2101  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2102  << NPSMEFTd6Vars_LFU_QFU[i] << std::endl;
2103  return false;
2104  }
2105  }
2106  }
2107 
2108  //} else if (FlagLeptonUniversal && !FlagQuarkUniversal) {
2109  //} else if (!FlagLeptonUniversal && FlagQuarkUniversal) {
2110  } else if (!FlagLeptonUniversal && !FlagQuarkUniversal) {
2111  if (FlagRotateCHWCHB) {
2112  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2113  if (DPars.find(NPSMEFTd6VarsRot[i]) == DPars.end()) {
2114  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter"
2115  << NPSMEFTd6VarsRot[i] << std::endl;
2116  return false;
2117  }
2118  }
2119  } else {
2120  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2121  if (DPars.find(NPSMEFTd6Vars[i]) == DPars.end()) {
2122  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter"
2123  << NPSMEFTd6Vars[i] << std::endl;
2124  return false;
2125  }
2126  }
2127  }
2128 
2129  } else
2130  throw std::runtime_error("Error in NPSMEFTd6::CheckParameters()");
2131 
2132  return (NPbase::CheckParameters(DPars));
2133 }
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPSMEFTd6.h:3922
std::map< std::string, double > DPars
Definition: Minimal.cpp:11
static const int NNPSMEFTd6Vars_LFU_QFU
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
Definition: NPSMEFTd6.h:777
static const std::string NPSMEFTd6Vars[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:765
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:3904
static const std::string NPSMEFTd6Vars_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:784
static const std::string NPSMEFTd6VarsRot_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:791
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPSMEFTd6.h:3916
virtual bool CheckParameters(const std::map< std::string, double > &DPars)
A method to check if all the mandatory parameters for StandardModel have been provided in model initi...
static const int NNPSMEFTd6Vars
The number of the model parameters in NPSMEFTd6.
Definition: NPSMEFTd6.h:759
static const std::string NPSMEFTd6VarsRot[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:771

◆ CHF1_diag()

double NPSMEFTd6::CHF1_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(1)})_{FF} \(\)

Definition at line 2172 of file NPSMEFTd6.cpp.

2173 {
2174  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2175  return CHL1_11;
2176  else if (F.is("NEUTRINO_2") || F.is("MU"))
2177  return CHL1_22;
2178  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2179  return CHL1_33;
2180  else if (F.is("UP") || F.is("DOWN"))
2181  return CHQ1_11;
2182  else if (F.is("CHARM") || F.is("STRANGE"))
2183  return CHQ1_22;
2184  else if (F.is("TOP") || F.is("BOTTOM"))
2185  return CHQ1_33;
2186  else
2187  throw std::runtime_error("NPSMEFTd6::CHF1_diag(): wrong argument");
2188 }
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
bool is(std::string name_i) const
Definition: Particle.cpp:23
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471

◆ CHF3_diag()

double NPSMEFTd6::CHF3_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(3)})_{FF} \(\)

Definition at line 2190 of file NPSMEFTd6.cpp.

2191 {
2192  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2193  return CHL3_11;
2194  else if (F.is("NEUTRINO_2") || F.is("MU"))
2195  return CHL3_22;
2196  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2197  return CHL3_33;
2198  else if (F.is("UP") || F.is("DOWN"))
2199  return CHQ3_11;
2200  else if (F.is("CHARM") || F.is("STRANGE"))
2201  return CHQ3_22;
2202  else if (F.is("TOP") || F.is("BOTTOM"))
2203  return CHQ3_33;
2204  else
2205  throw std::runtime_error("NPSMEFTd6::CHF3_diag(): wrong argument");
2206 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
bool is(std::string name_i) const
Definition: Particle.cpp:23

◆ CHf_diag()

double NPSMEFTd6::CHf_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{Hf})_{ff} \(\)

Definition at line 2208 of file NPSMEFTd6.cpp.

2209 {
2210  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2211  return 0.0;
2212  else if (f.is("ELECTRON"))
2213  return CHe_11;
2214  else if (f.is("MU"))
2215  return CHe_22;
2216  else if (f.is("TAU"))
2217  return CHe_33;
2218  else if (f.is("UP"))
2219  return CHu_11;
2220  else if (f.is("CHARM"))
2221  return CHu_22;
2222  else if (f.is("TOP"))
2223  return CHu_33;
2224  else if (f.is("DOWN"))
2225  return CHd_11;
2226  else if (f.is("STRANGE"))
2227  return CHd_22;
2228  else if (f.is("BOTTOM"))
2229  return CHd_33;
2230  else
2231  throw std::runtime_error("NPSMEFTd6::CHf_diag(): wrong argument");
2232 }
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3494
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
bool is(std::string name_i) const
Definition: Particle.cpp:23
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465

◆ CHud_diag()

gslpp::complex NPSMEFTd6::CHud_diag ( const Particle  u) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.

Parameters
[in]ua quark
Returns
\((\)C_{Hud})_{ud} \(\)

Definition at line 2234 of file NPSMEFTd6.cpp.

2235 {
2236  if (!u.is("QUARK") || u.getIndex() % 2 != 0)
2237  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2238 
2239  if (u.is("UP"))
2240  return gslpp::complex(CHud_11r, CHud_11i, false);
2241  else if (u.is("CHARM"))
2242  return gslpp::complex(CHud_22r, CHud_22i, false);
2243  else if (u.is("TOP"))
2244  return gslpp::complex(CHud_22r, CHud_33i, false);
2245  else
2246  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2247 }
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3510
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3518
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3513
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3516
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3507
int getIndex() const
Definition: Particle.h:160
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35

◆ CLL_bottom()

double NPSMEFTd6::CLL_bottom ( ) const

Definition at line 13296 of file NPSMEFTd6.cpp.

13297 {
13299 }
double CLQ1_1133
Definition: NPSMEFTd6.h:3596
double CLQ1_3311
Definition: NPSMEFTd6.h:3596
double CLQ3_1133
Definition: NPSMEFTd6.h:3601
double CLQ3_3311
Definition: NPSMEFTd6.h:3601

◆ CLL_charm()

double NPSMEFTd6::CLL_charm ( ) const

Definition at line 13286 of file NPSMEFTd6.cpp.

13287 {
13289 }
double CLQ3_1122
Definition: NPSMEFTd6.h:3600
double CLQ1_2211
Definition: NPSMEFTd6.h:3595
double CLQ1_1122
Definition: NPSMEFTd6.h:3595
double CLQ3_2211
Definition: NPSMEFTd6.h:3600

◆ CLL_down()

double NPSMEFTd6::CLL_down ( ) const

Definition at line 13281 of file NPSMEFTd6.cpp.

13282 {
13283  return (CLQ1_1111+CLQ3_1111);
13284 }
double CLQ3_1111
Definition: NPSMEFTd6.h:3599
double CLQ1_1111
Definition: NPSMEFTd6.h:3594

◆ CLL_mu()

double NPSMEFTd6::CLL_mu ( ) const

Definition at line 13266 of file NPSMEFTd6.cpp.

13267 {
13268  return (CLL_1122 + CLL_2211 + CLL_1221 + CLL_2112);
13269 }
double CLL_1221
Definition: NPSMEFTd6.h:3592
double CLL_2211
Definition: NPSMEFTd6.h:3592
double CLL_2112
Definition: NPSMEFTd6.h:3592
double CLL_1122
Definition: NPSMEFTd6.h:3592

◆ CLL_strange()

double NPSMEFTd6::CLL_strange ( ) const

Definition at line 13291 of file NPSMEFTd6.cpp.

13292 {
13294 }
double CLQ3_1122
Definition: NPSMEFTd6.h:3600
double CLQ1_2211
Definition: NPSMEFTd6.h:3595
double CLQ1_1122
Definition: NPSMEFTd6.h:3595
double CLQ3_2211
Definition: NPSMEFTd6.h:3600

◆ CLL_tau()

double NPSMEFTd6::CLL_tau ( ) const

Definition at line 13271 of file NPSMEFTd6.cpp.

13272 {
13273  return (CLL_1133 + CLL_3311 + CLL_1331 + CLL_3113);
13274 }
double CLL_1331
Definition: NPSMEFTd6.h:3593
double CLL_1133
Definition: NPSMEFTd6.h:3593
double CLL_3113
Definition: NPSMEFTd6.h:3593
double CLL_3311
Definition: NPSMEFTd6.h:3593

◆ CLL_up()

double NPSMEFTd6::CLL_up ( ) const

Definition at line 13276 of file NPSMEFTd6.cpp.

13277 {
13278  return (CLQ1_1111-CLQ3_1111);
13279 }
double CLQ3_1111
Definition: NPSMEFTd6.h:3599
double CLQ1_1111
Definition: NPSMEFTd6.h:3594

◆ CLR_bottom()

double NPSMEFTd6::CLR_bottom ( ) const

Definition at line 13331 of file NPSMEFTd6.cpp.

13332 {
13333  return (CLd_1133+CLd_3311);
13334 }
double CLd_1133
Definition: NPSMEFTd6.h:3625
double CLd_3311
Definition: NPSMEFTd6.h:3625

◆ CLR_charm()

double NPSMEFTd6::CLR_charm ( ) const

Definition at line 13321 of file NPSMEFTd6.cpp.

13322 {
13323  return (CLu_1122+CLu_2211);
13324 }
double CLu_2211
Definition: NPSMEFTd6.h:3620
double CLu_1122
Definition: NPSMEFTd6.h:3620

◆ CLR_down()

double NPSMEFTd6::CLR_down ( ) const

Definition at line 13316 of file NPSMEFTd6.cpp.

13317 {
13318  return (CLd_1111);
13319 }
double CLd_1111
Definition: NPSMEFTd6.h:3623

◆ CLR_mu()

double NPSMEFTd6::CLR_mu ( ) const

Definition at line 13301 of file NPSMEFTd6.cpp.

13302 {
13303  return (CLe_1122+CLe_2211);
13304 }
double CLe_1122
Definition: NPSMEFTd6.h:3617
double CLe_2211
Definition: NPSMEFTd6.h:3617

◆ CLR_strange()

double NPSMEFTd6::CLR_strange ( ) const

Definition at line 13326 of file NPSMEFTd6.cpp.

13327 {
13328  return (CLd_1122+CLd_2211);
13329 }
double CLd_1122
Definition: NPSMEFTd6.h:3624
double CLd_2211
Definition: NPSMEFTd6.h:3624

◆ CLR_tau()

double NPSMEFTd6::CLR_tau ( ) const

Definition at line 13306 of file NPSMEFTd6.cpp.

13307 {
13308  return (CLe_1133+CLe_3311);
13309 }
double CLe_3311
Definition: NPSMEFTd6.h:3618
double CLe_1133
Definition: NPSMEFTd6.h:3618

◆ CLR_up()

double NPSMEFTd6::CLR_up ( ) const

Definition at line 13311 of file NPSMEFTd6.cpp.

13312 {
13313  return (CLu_1111);
13314 }
double CLu_1111
Definition: NPSMEFTd6.h:3619

◆ computeGammaTotalRatio()

double NPSMEFTd6::computeGammaTotalRatio ( ) const
virtual

The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 9931 of file NPSMEFTd6.cpp.

9932 {
9933  double width = 1.0;
9934 
9935  width += dGammaHTotR1;
9936 
9937  if (FlagQuadraticTerms) {
9938  //Add contributions that are quadratic in the effective coefficients
9939  width += dGammaHTotR2;
9940  }
9941 
9942  if (width < 0) return std::numeric_limits<double>::quiet_NaN();
9943 
9944  return width;
9945 
9946 }
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ CRL_bottom()

double NPSMEFTd6::CRL_bottom ( ) const

Definition at line 13366 of file NPSMEFTd6.cpp.

13367 {
13368  return (CQe_1133+CQe_3311);
13369 }
double CQe_3311
Definition: NPSMEFTd6.h:3630
double CQe_1133
Definition: NPSMEFTd6.h:3630

◆ CRL_charm()

double NPSMEFTd6::CRL_charm ( ) const

Definition at line 13356 of file NPSMEFTd6.cpp.

13357 {
13358  return (CQe_1122+CQe_2211);
13359 }
double CQe_2211
Definition: NPSMEFTd6.h:3629
double CQe_1122
Definition: NPSMEFTd6.h:3629

◆ CRL_down()

double NPSMEFTd6::CRL_down ( ) const

Definition at line 13351 of file NPSMEFTd6.cpp.

13352 {
13353  return (CQe_1111);
13354 }
double CQe_1111
Definition: NPSMEFTd6.h:3628

◆ CRL_mu()

double NPSMEFTd6::CRL_mu ( ) const

Definition at line 13336 of file NPSMEFTd6.cpp.

13337 {
13338  return (CLe_1122+CLe_2211);
13339 }
double CLe_1122
Definition: NPSMEFTd6.h:3617
double CLe_2211
Definition: NPSMEFTd6.h:3617

◆ CRL_strange()

double NPSMEFTd6::CRL_strange ( ) const

Definition at line 13361 of file NPSMEFTd6.cpp.

13362 {
13363  return (CQe_1122+CQe_2211);
13364 }
double CQe_2211
Definition: NPSMEFTd6.h:3629
double CQe_1122
Definition: NPSMEFTd6.h:3629

◆ CRL_tau()

double NPSMEFTd6::CRL_tau ( ) const

Definition at line 13341 of file NPSMEFTd6.cpp.

13342 {
13343  return (CLe_1133+CLe_3311);
13344 }
double CLe_3311
Definition: NPSMEFTd6.h:3618
double CLe_1133
Definition: NPSMEFTd6.h:3618

◆ CRL_up()

double NPSMEFTd6::CRL_up ( ) const

Definition at line 13346 of file NPSMEFTd6.cpp.

13347 {
13348  return (CQe_1111);
13349 }
double CQe_1111
Definition: NPSMEFTd6.h:3628

◆ CRR_bottom()

double NPSMEFTd6::CRR_bottom ( ) const

Definition at line 13402 of file NPSMEFTd6.cpp.

13403 {
13404  return (Ced_1133+Ced_3311);
13405 }
double Ced_1133
Definition: NPSMEFTd6.h:3613
double Ced_3311
Definition: NPSMEFTd6.h:3613

◆ CRR_charm()

double NPSMEFTd6::CRR_charm ( ) const

Definition at line 13392 of file NPSMEFTd6.cpp.

13393 {
13394  return (Ceu_1122+Ceu_2211);
13395 }
double Ceu_1122
Definition: NPSMEFTd6.h:3608
double Ceu_2211
Definition: NPSMEFTd6.h:3608

◆ CRR_down()

double NPSMEFTd6::CRR_down ( ) const

Definition at line 13387 of file NPSMEFTd6.cpp.

13388 {
13389  return (Ced_1111);
13390 }
double Ced_1111
Definition: NPSMEFTd6.h:3611

◆ CRR_mu()

double NPSMEFTd6::CRR_mu ( ) const

Definition at line 13371 of file NPSMEFTd6.cpp.

13372 {
13373  return (Cee_1122+Cee_2211);
13374 }
double Cee_2211
Definition: NPSMEFTd6.h:3605
double Cee_1122
Definition: NPSMEFTd6.h:3605

◆ CRR_strange()

double NPSMEFTd6::CRR_strange ( ) const

Definition at line 13397 of file NPSMEFTd6.cpp.

13398 {
13399  return (Ced_1122+Ced_2211);
13400 }
double Ced_2211
Definition: NPSMEFTd6.h:3612
double Ced_1122
Definition: NPSMEFTd6.h:3612

◆ CRR_tau()

double NPSMEFTd6::CRR_tau ( ) const

Definition at line 13376 of file NPSMEFTd6.cpp.

13377 {
13378  return (Cee_1133+Cee_3311);
13379 }
double Cee_3311
Definition: NPSMEFTd6.h:3606
double Cee_1133
Definition: NPSMEFTd6.h:3606

◆ CRR_up()

double NPSMEFTd6::CRR_up ( ) const

Definition at line 13382 of file NPSMEFTd6.cpp.

13383 {
13384  return (Ceu_1111);
13385 }
double Ceu_1111
Definition: NPSMEFTd6.h:3607

◆ cZBox_HB()

double NPSMEFTd6::cZBox_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\Box}\)

Reimplemented from NPbase.

Definition at line 12834 of file NPSMEFTd6.cpp.

12835 {
12836  double ciHB;
12837 
12838  ciHB = (sW2_tree/eeMz2)*( DeltaGF() + 0.5*CHD*v2_over_LambdaNP2 );
12839 
12840  ciHB = ciHB + 0.5*(sW2_tree/eeMz)*(CDHB / cW_tree + CDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
12841 
12842  return ciHB;
12843 }
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804

◆ cZga_HB()

double NPSMEFTd6::cZga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\gamma}\)

Reimplemented from NPbase.

Definition at line 12858 of file NPSMEFTd6.cpp.

12859 {
12860  double ciHB;
12861 
12862  ciHB = (sW2_tree*cW2_tree/eeMz2)*( 4.0*CHW - 4.0*CHB - (2.0*(cW2_tree-sW2_tree)/sW_tree/cW_tree)*CHWB )*v2_over_LambdaNP2;
12863 
12864  ciHB = ciHB + 0.5*(sW_tree*cW_tree/eeMz)*(CDHB / sW_tree - CDHW / cW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
12865 
12866  return ciHB;
12867 }
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804

◆ cZZ_HB()

double NPSMEFTd6::cZZ_HB ( ) const
virtual

The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{zz}\)

Reimplemented from NPbase.

Definition at line 12846 of file NPSMEFTd6.cpp.

12847 {
12848  double ciHB;
12849 
12851 
12852  ciHB = ciHB - (sW2_tree*cW2_tree/eeMz)*(CDHB / cW_tree + CDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
12853 
12854  return ciHB;
12855 }
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804

◆ deltaa0()

double NPSMEFTd6::deltaa0 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(0)/\alpha(0)\)

Definition at line 2476 of file NPSMEFTd6.cpp.

2477 {
2478  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2479  return ( (aleMz - 0.0072973525664) / 0.0072973525664 );
2480 }
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802

◆ deltaa02()

double NPSMEFTd6::deltaa02 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(0)/\alpha(0))^2\)

Definition at line 2482 of file NPSMEFTd6.cpp.

2483 {
2484  return ( 0.0 );
2485 }

◆ deltaaMZ()

double NPSMEFTd6::deltaaMZ ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\)

Definition at line 2465 of file NPSMEFTd6.cpp.

2466 {
2467  // Ref. value from SM EW fit 2018
2468  return ( (aleMz - 0.007754941997887603) / 0.007754941997887603 );
2469 }
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802

◆ deltaaMZ2()

double NPSMEFTd6::deltaaMZ2 ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\)

Definition at line 2471 of file NPSMEFTd6.cpp.

2472 {
2473  return ( 0.0 );
2474 }

◆ deltaaSMZ()

double NPSMEFTd6::deltaaSMZ ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\)

Definition at line 2487 of file NPSMEFTd6.cpp.

2488 {
2489  // Ref. value from SM EW fit 2018
2490  return ( (AlsMz - 0.1180) / 0.1180 );
2491 }
double AlsMz
The strong coupling constant at the Z-boson mass, .

◆ deltaaSMZ2()

double NPSMEFTd6::deltaaSMZ2 ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\)

Definition at line 2493 of file NPSMEFTd6.cpp.

2494 {
2495  return ( 0.0 );
2496 }

◆ deltacZ_HB()

double NPSMEFTd6::deltacZ_HB ( ) const
virtual

The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta c_z\)

Reimplemented from NPbase.

Definition at line 12824 of file NPSMEFTd6.cpp.

12825 {
12826  double ciHB;
12827 
12828  ciHB = delta_h - (3.0/2.0)*DeltaGF();
12829 
12830  return ciHB;
12831 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356

◆ deltaG1_hWW()

double NPSMEFTd6::deltaG1_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2692 of file NPSMEFTd6.cpp.

2693 {
2694  return (( 2.0 * CHW - sqrt( M_PI * aleMz ) * CDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2695 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG1_hZA()

double NPSMEFTd6::deltaG1_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2730 of file NPSMEFTd6.cpp.

2731 {
2732  return ( (delta_AZ + 0.5 * sqrt( M_PI * aleMz ) * (CDHB / sW_tree - CDHW / cW_tree) * v2_over_LambdaNP2 )/ v());
2733 }
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3823
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG1_hZARatio()

double NPSMEFTd6::deltaG1_hZARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HZA}^{(1)}/g_{HZA}^{(1),SM}\)

Reimplemented from NPbase.

Definition at line 2735 of file NPSMEFTd6.cpp.

2736 {
2737  double m_t = mtpole;
2738  double m_b = quarks[BOTTOM].getMass();
2739  double m_c = quarks[CHARM].getMass();
2740  double m_tau = leptons[TAU].getMass();
2741  double m_mu = leptons[MU].getMass();
2742 
2743  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
2744 
2745  double Qt = quarks[TOP].getCharge();
2746  double Qb = quarks[BOTTOM].getCharge();
2747  double Qc = quarks[CHARM].getCharge();
2748  double Qtau = leptons[TAU].getCharge();
2749  double Qmu = leptons[MU].getCharge();
2750 
2751  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
2752  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
2753  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
2754  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
2755  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
2756  double tau_W = 4.0 * M_w_2 / mHl / mHl;
2757 
2758  double lambda_t = 4.0 * m_t * m_t / Mz / Mz;
2759  double lambda_b = 4.0 * m_b * m_b / Mz / Mz;
2760  double lambda_c = 4.0 * m_c * m_c / Mz / Mz;
2761  double lambda_tau = 4.0 * m_tau * m_tau / Mz / Mz;
2762  double lambda_mu = 4.0 * m_mu * m_mu / Mz / Mz;
2763  double lambda_W = 4.0 * M_w_2 / Mz / Mz;
2764  double alpha2 = sqrt(2.0)*GF*M_w_2 / M_PI;
2765  double aPiv = sqrt(ale*alpha2) / 4.0 / M_PI / v();
2766 
2767 // mod. of Higgs couplings
2768  gslpp::complex gSM, dg;
2769  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
2770  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
2771  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
2772  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
2773  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
2774  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
2775 
2776 // mod of EW vector couplings vf =2 gvf
2777  double vSMt = 2.0*(quarks[TOP].getIsospin()) - 4.0 * Qt * sW2_tree;
2778  double vSMb = 2.0*(quarks[BOTTOM].getIsospin()) - 4.0 * Qb * sW2_tree;
2779  double vSMc = 2.0*(quarks[CHARM].getIsospin()) - 4.0 * Qc * sW2_tree;
2780  double vSMtau = 2.0*(leptons[TAU].getIsospin()) - 4.0 * Qtau * sW2_tree;
2781  double vSMmu = 2.0*(leptons[MU].getIsospin()) - 4.0 * Qmu * sW2_tree;
2782 
2783  double dvSMt = cLHd6 * 2.0*deltaGV_f(quarks[TOP]);
2784  double dvSMb = cLHd6 * 2.0*deltaGV_f(quarks[BOTTOM]);
2785  double dvSMc = cLHd6 * 2.0*deltaGV_f(quarks[CHARM]);
2786  double dvSMtau = cLHd6 * 2.0*deltaGV_f(leptons[TAU]);
2787  double dvSMmu = cLHd6 * 2.0*deltaGV_f(leptons[MU]);
2788 
2789  double deltaloc = deltaG1_hZA();
2790 
2791  gSM = -aPiv * ((3.0*vSMt*Qt*AHZga_f(tau_t,lambda_t) +
2792  3.0*vSMb*Qb*AHZga_f(tau_b,lambda_b) +
2793  3.0*vSMc*Qc*AHZga_f(tau_c,lambda_c) +
2794  vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
2795  vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
2796  AHZga_W(tau_W,lambda_W));
2797 
2798  dg = deltaloc/gSM - (aPiv/gSM) * (
2799  (3.0*vSMt*dKappa_t*Qt*AHZga_f(tau_t,lambda_t) +
2800  3.0*vSMb*dKappa_b*Qb*AHZga_f(tau_b,lambda_b) +
2801  3.0*vSMc*dKappa_c*Qc*AHZga_f(tau_c,lambda_c)+
2802  dKappa_tau*vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
2803  dKappa_mu*vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
2804  dKappa_W*AHZga_W(tau_W,lambda_W) +
2805  (3.0*dvSMt*Qt*AHZga_f(tau_t,lambda_t) +
2806  3.0*dvSMb*Qb*AHZga_f(tau_b,lambda_b) +
2807  3.0*dvSMc*Qc*AHZga_f(tau_c,lambda_c)+
2808  dvSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
2809  dvSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree
2810  );
2811 
2812  return dg.real();
2813 }
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
StandardModel trueSM
Definition: NPbase.h:1902
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double ale
The fine-structure constant .
double GF
The Fermi constant in .
virtual double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
Definition: NPSMEFTd6.cpp:2600
double mHl
The Higgs mass in GeV.
gslpp::complex AHZga_W(const double tau, const double lambda) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3044
Definition: QCD.h:619
double Mz
The mass of the boson in GeV.
Definition: QCD.h:607
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
virtual double Mw() const
The SM prediction for the -boson mass in the on-shell scheme, .
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
Particle leptons[6]
An array of Particle objects for the leptons.
virtual double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2730
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
Definition: QCD.h:605
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
virtual double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2702
gslpp::complex AHZga_f(const double tau, const double lambda) const
Fermionic loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3039
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
complex sqrt(const complex &z)

◆ deltaG1_hZZ()

double NPSMEFTd6::deltaG1_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(1)}\)

Reimplemented from NPbase.

Definition at line 2713 of file NPSMEFTd6.cpp.

2714 {
2715  return ( (delta_ZZ - 0.5 * sqrt( M_PI * aleMz ) * (CDHB / cW_tree + CDHW / sW_tree) * v2_over_LambdaNP2 )/ v());
2716 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3821
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltag1ZNP()

double NPSMEFTd6::deltag1ZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).

Returns
\(\delta g_{1,Z}\)

Reimplemented from NPbase.

Definition at line 12190 of file NPSMEFTd6.cpp.

12191 {
12192  double NPdirect, NPindirect;
12193 
12194  /* From own calculations. Agrees with with LHCHXWG-INT-2015-001 for common interactions */
12195  NPdirect = sW_tree / sqrt( 4.0 * M_PI * aleMz );
12196  NPdirect = - NPdirect * (Mz * Mz / v () / v() ) * CDHW * v2_over_LambdaNP2;
12197 
12198  NPindirect = - 1.0 / (cW2_tree-sW2_tree);
12199 
12200  NPindirect = NPindirect * (sW_tree * CHWB / cW_tree
12201  + 0.25 * CHD ) * v2_over_LambdaNP2
12202  + 0.5 * NPindirect * DeltaGF() ;
12203 
12204  return NPdirect + NPindirect + dg1Z ;
12205 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double dg1Z
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3796
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double Mz
The mass of the boson in GeV.
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG2_hWW()

double NPSMEFTd6::deltaG2_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(2)}\)

Reimplemented from NPbase.

Definition at line 2697 of file NPSMEFTd6.cpp.

2698 {
2699  return ( - sqrt( M_PI * aleMz ) * ( CDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2700 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG2_hZA()

double NPSMEFTd6::deltaG2_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(2)}\)

Reimplemented from NPbase.

Definition at line 2815 of file NPSMEFTd6.cpp.

2816 {
2817  return ( sqrt( M_PI * aleMz ) * ( CDHB / sW_tree - CDHW / cW_tree ) * v2_over_LambdaNP2 / v());
2818 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG2_hZZ()

double NPSMEFTd6::deltaG2_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(2)}\)

Reimplemented from NPbase.

Definition at line 2718 of file NPSMEFTd6.cpp.

2719 {
2720  return ( - sqrt( M_PI * aleMz ) * ( CDHB / cW_tree + CDHW / sW_tree ) * v2_over_LambdaNP2 / v());
2721 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltaG3_hWW()

double NPSMEFTd6::deltaG3_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).

Returns
\(\delta g_{HWW}^{(3)}\)

Reimplemented from NPbase.

Definition at line 2702 of file NPSMEFTd6.cpp.

2703 {
2704  double NPindirect;
2705 
2706  NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
2707  * (delta_h - 1.0 / 2.0 / (cW2_tree - sW2_tree)
2708  * ((4.0 * sW_tree * cW_tree * CHWB + cW2_tree * CHD) * v2_over_LambdaNP2 + DeltaGF()));
2709 
2710  return NPindirect;
2711 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double Mz
The mass of the boson in GeV.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440

◆ deltaG3_hZZ()

double NPSMEFTd6::deltaG3_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).

Returns
\(\delta g_{HZZ}^{(3)}\)

Reimplemented from NPbase.

Definition at line 2723 of file NPSMEFTd6.cpp.

2724 {
2725  double NPindirect = Mz * Mz / v() * (-0.5 * CHD * v2_over_LambdaNP2 + delta_h - 0.5 * DeltaGF());
2726  double NPdirect = Mz * Mz / v() * CHD * v2_over_LambdaNP2;
2727  return (NPindirect + NPdirect);
2728 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double Mz
The mass of the boson in GeV.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...

◆ deltag3G()

double NPSMEFTd6::deltag3G ( ) const

The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).

Returns
\(\delta g_{3G}\)

Definition at line 2975 of file NPSMEFTd6.cpp.

2976 {
2977  /* Set to 0. for the moment */
2978 
2979  return 0.;
2980 }

◆ deltaG_Aff()

gslpp::complex NPSMEFTd6::deltaG_Aff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Aff}\)

Definition at line 2968 of file NPSMEFTd6.cpp.

2969 {
2970  /* Set to 0. for the moment */
2971 
2972  return 0.;
2973 }

◆ deltaG_Gff()

gslpp::complex NPSMEFTd6::deltaG_Gff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Gff}\)

Definition at line 2954 of file NPSMEFTd6.cpp.

2955 {
2956  /* Set to 0. for the moment */
2957 
2958  return 0.;
2959 }

◆ deltaG_hAA()

double NPSMEFTd6::deltaG_hAA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HAA}\)

Reimplemented from NPbase.

Definition at line 2820 of file NPSMEFTd6.cpp.

2821 {
2822  return (delta_AA / v());
2823 }
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3822
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...

◆ deltaG_hAARatio()

double NPSMEFTd6::deltaG_hAARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HAA}/g_{HAA}^SM}\)

Reimplemented from NPbase.

Definition at line 2825 of file NPSMEFTd6.cpp.

2826 {
2827  double m_t = mtpole;
2828  double m_b = quarks[BOTTOM].getMass();
2829  double m_c = quarks[CHARM].getMass();
2830  double m_tau = leptons[TAU].getMass();
2831  double m_mu = leptons[MU].getMass();
2832 
2833  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
2834 
2835  double Qt = quarks[TOP].getCharge();
2836  double Qb = quarks[BOTTOM].getCharge();
2837  double Qc = quarks[CHARM].getCharge();
2838  double Qtau = leptons[TAU].getCharge();
2839  double Qmu = leptons[MU].getCharge();
2840 
2841  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
2842  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
2843  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
2844  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
2845  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
2846  double tau_W = 4.0 * M_w_2 / mHl / mHl;
2847 
2848  double aPiv = ale / 8.0 / M_PI / v();
2849  gslpp::complex gSM, dg;
2850  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
2851  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
2852  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
2853  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
2854  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
2855  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
2856 
2857  double deltaloc = deltaG_hAA();
2858 
2859  gSM = aPiv * (3.0*Qt*Qt*AH_f(tau_t) +
2860  3.0*Qb*Qb*AH_f(tau_b) +
2861  3.0*Qc*Qc*AH_f(tau_c) +
2862  Qtau*Qtau*AH_f(tau_tau) +
2863  Qmu*Qmu*AH_f(tau_mu) +
2864  AH_W(tau_W));
2865 
2866  dg = deltaloc/gSM + (aPiv/gSM) * (
2867  3.0*Qt*Qt*dKappa_t*AH_f(tau_t) +
2868  3.0*Qb*Qb*dKappa_b*AH_f(tau_b) +
2869  3.0*Qc*Qc*dKappa_c*AH_f(tau_c) +
2870  dKappa_tau*Qtau*Qtau*AH_f(tau_tau) +
2871  dKappa_mu*Qmu*Qmu*AH_f(tau_mu) +
2872  dKappa_W*AH_W(tau_W)
2873  );
2874 
2875  return dg.real();
2876 }
const double & real() const
gslpp::complex AH_W(const double tau) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3034
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
StandardModel trueSM
Definition: NPbase.h:1902
double ale
The fine-structure constant .
double mHl
The Higgs mass in GeV.
Definition: QCD.h:619
Definition: QCD.h:607
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
virtual double Mw() const
The SM prediction for the -boson mass in the on-shell scheme, .
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
Particle leptons[6]
An array of Particle objects for the leptons.
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3029
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
virtual double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2820
Definition: QCD.h:605
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
virtual double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2702
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaG_hAff()

gslpp::complex NPSMEFTd6::deltaG_hAff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hAff}\)

Definition at line 2947 of file NPSMEFTd6.cpp.

2948 {
2949  /* Set to 0. for the moment */
2950 
2951  return 0.;
2952 }

◆ deltaG_hff()

gslpp::complex NPSMEFTd6::deltaG_hff ( const Particle  p) const
virtual

The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Hff}\)

Reimplemented from NPbase.

Definition at line 2878 of file NPSMEFTd6.cpp.

2879 {
2880  /* The effects of the RG running are neglected. */
2881  double mf;
2882  if (p.is("TOP"))
2883  //mf = p.getMass(); // m_t(m_t)
2884  mf = mtpole; // pole mass
2885  else
2886  mf = p.getMass();
2887  gslpp::complex CfH = CfH_diag(p);
2888  return (-mf / v() * (delta_h - 0.5 * DeltaGF())
2889  + CfH * v2_over_LambdaNP2 / sqrt(2.0));
2890 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
gslpp::complex CfH_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f...
Definition: NPSMEFTd6.cpp:2249
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
bool is(std::string name_i) const
Definition: Particle.cpp:23
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
complex sqrt(const complex &z)

◆ deltaG_hGff()

gslpp::complex NPSMEFTd6::deltaG_hGff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hGff}\)

Definition at line 2933 of file NPSMEFTd6.cpp.

2934 {
2935  /* Set to 0. for the moment */
2936 
2937  return 0.;
2938 }

◆ deltaG_hgg()

double NPSMEFTd6::deltaG_hgg ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).

Returns
\(\delta g_{HGG}\)

Reimplemented from NPbase.

Definition at line 2665 of file NPSMEFTd6.cpp.

2666 {
2667  return (CHG * v2_over_LambdaNP2 / v());
2668 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...

◆ deltaG_hggRatio()

double NPSMEFTd6::deltaG_hggRatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HGG}/g_{HGG}^SM}\)

Reimplemented from NPbase.

Definition at line 2670 of file NPSMEFTd6.cpp.

2671 {
2672  double m_t = mtpole;
2673  double m_b = quarks[BOTTOM].getMass();
2674  double m_c = quarks[CHARM].getMass();
2675  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
2676  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
2677  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
2678  double aSPiv = AlsMz / 16.0 / M_PI / v();
2679  gslpp::complex gSM, dg;
2680  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
2681  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
2682  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
2683  double deltaloc = deltaG_hgg();
2684 
2685  gSM = aSPiv * (AH_f(tau_t) + AH_f(tau_b) + AH_f(tau_c));
2686 
2687  dg = deltaloc/gSM + (aSPiv/gSM) * (dKappa_t*AH_f(tau_t) + dKappa_b*AH_f(tau_b) + dKappa_c*AH_f(tau_c));
2688 
2689  return dg.real();
2690 }
virtual double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2665
const double & real() const
double AlsMz
The strong coupling constant at the Z-boson mass, .
double mHl
The Higgs mass in GeV.
Definition: QCD.h:619
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3029
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaG_hhhRatio()

double NPSMEFTd6::deltaG_hhhRatio ( ) const
virtual

The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.

Returns
\(\delta g_{HHH}/g_{HHH}^SM}\)

Reimplemented from NPbase.

Definition at line 2892 of file NPSMEFTd6.cpp.

2893 {
2894  double dg;
2895 
2896  dg = -0.5 * DeltaGF() + 3.0 * delta_h - 2.0 * CH * v2_over_LambdaNP2 * v2/mHl/mHl;
2897 
2898  return dg;
2899 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
double CH
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3443
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double mHl
The Higgs mass in GeV.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:3800

◆ deltaG_hZff()

gslpp::complex NPSMEFTd6::deltaG_hZff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hZff}\)

Definition at line 2940 of file NPSMEFTd6.cpp.

2941 {
2942  /* Set to 0. for the moment */
2943 
2944  return 0.;
2945 }

◆ deltaG_Zff()

gslpp::complex NPSMEFTd6::deltaG_Zff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Zff}\)

Definition at line 2961 of file NPSMEFTd6.cpp.

2962 {
2963  /* Set to 0. for the moment */
2964 
2965  return 0.;
2966 }

◆ deltaGA_f()

double NPSMEFTd6::deltaGA_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_A^f\)

Reimplemented from NPbase.

Definition at line 2605 of file NPSMEFTd6.cpp.

2606 {
2607  return (deltaGL_f(p) - deltaGR_f(p));
2608 }
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPSMEFTd6.cpp:2610
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPSMEFTd6.cpp:2625

◆ deltaGamma_W()

double NPSMEFTd6::deltaGamma_W ( ) const
virtual

The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).

Returns
\(\delta \Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 2558 of file NPSMEFTd6.cpp.

2559 {
2560  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
2561  double GammaW_tree = (3.0 + 2.0 * Nc) * G0;
2562 
2563  return (- 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
2564  *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
2566  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF())
2567  + 2.0 * G0 * (CHL3_11 + CHL3_22 + CHL3_33 + Nc*(CHQ3_11 + CHQ3_22)) * v2_over_LambdaNP2);
2568 // + 2.0 * GammaW_tree / 3.0 * (CHL3_11 + CHQ3_11 + CHQ3_22) * v2_over_LambdaNP2);
2569 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
complex pow(const complex &z1, const complex &z2)
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double GF
The Fermi constant in .
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double Mz
The mass of the boson in GeV.
double Nc
The number of colours.
Definition: QCD.h:1220
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
complex sqrt(const complex &z)

◆ deltaGamma_Wff()

double NPSMEFTd6::deltaGamma_Wff ( const Particle  fi,
const Particle  fj 
) const
virtual

The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\delta \Gamma_W^{ff}\) in GeV

Reimplemented from NPbase.

Definition at line 2524 of file NPSMEFTd6.cpp.

2525 {
2526  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
2527  double deltaGamma_Wij;
2528  double GammaW_tree;
2529  double CHF3ij;
2530 
2531  if (fj.getIndex() - fi.getIndex() == 1)
2532  CHF3ij = CHF3_diag(fi);
2533  else
2534  CHF3ij = 0.;
2535 
2536  if (fi.is("QUARK")) {
2537  GammaW_tree = Nc * G0;
2538  } else {
2539  GammaW_tree = G0;
2540  }
2541 
2542  deltaGamma_Wij = - 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
2543  *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
2545  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF());
2546 
2547  deltaGamma_Wij = deltaGamma_Wij + 2.0 * GammaW_tree * CHF3ij * v2_over_LambdaNP2;
2548 
2549  return deltaGamma_Wij;
2550 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
complex pow(const complex &z1, const complex &z2)
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double GF
The Fermi constant in .
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double Mz
The mass of the boson in GeV.
double Nc
The number of colours.
Definition: QCD.h:1220
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
int getIndex() const
Definition: Particle.h:160
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
bool is(std::string name_i) const
Definition: Particle.cpp:23
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2190
complex sqrt(const complex &z)

◆ deltaGammaHbbRatio1()

double NPSMEFTd6::deltaGammaHbbRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 11680 of file NPSMEFTd6.cpp.

11681 {
11682  double dwidth = 0.0;
11683 
11684  double C1 = 0.0;
11685 
11686  if (FlagLoopHd6) {
11687 
11688  dwidth = ( +121248. * CHbox / LambdaNP2
11689  -558.186 * CuH_33r / LambdaNP2
11690  -5027051. * CdH_33r / LambdaNP2
11691  -30312.1 * CHD / LambdaNP2
11692  -60624.1 * DeltaGF() / v() / v() );
11693 
11694  } else {
11695 
11696  dwidth = ( +121248. * CHbox / LambdaNP2
11697  -5050180. * CdH_33r / LambdaNP2
11698  -30312.1 * CHD / LambdaNP2
11699  -60624.1 * DeltaGF() / v() / v() );
11700  }
11701 
11702 // Linear contribution from Higgs self-coupling
11703  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11704 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11705  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11706 
11707  // Add modifications due to small variations of the SM parameters
11708  dwidth += cHSM * ( +1. * deltaGmu()
11709  -0.23 * deltaaSMZ()
11710  +1.007 * deltaMh()
11711  +0.001 * deltamt()
11712  +1.992 * deltamb() );
11713 
11714  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11715  dwidth += eHbbint + eHbbpar;
11716 
11717  return dwidth;
11718 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double eHbbpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3669
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2421
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHbbint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3668
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2487
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:3909
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHbbRatio2()

double NPSMEFTd6::deltaGammaHbbRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 11720 of file NPSMEFTd6.cpp.

11721 {
11722  double dwidth = 0.0;
11723 
11724 
11725  //Contributions that are quadratic in the effective coefficients
11726  return ( dwidth );
11727 
11728 }

◆ deltaGammaHccRatio1()

double NPSMEFTd6::deltaGammaHccRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 11615 of file NPSMEFTd6.cpp.

11616 {
11617  double dwidth = 0.0;
11618 
11619  double C1 = 0.0;
11620 
11621  if (FlagLoopHd6) {
11622 
11623  dwidth = ( +121248. * CHbox / LambdaNP2
11624  -16421890. * CuH_22r / LambdaNP2
11625  -992.159 * CuH_33r / LambdaNP2
11626  -30312.1 * CHD / LambdaNP2
11627  -60624.1 * DeltaGF() / v() / v() );
11628 
11629  } else {
11630 
11631  dwidth = ( +121248. * CHbox / LambdaNP2
11632  -16556668. * CuH_22r / LambdaNP2
11633  -30312.1 * CHD / LambdaNP2
11634  -60624.1 * DeltaGF() / v() / v() );
11635  }
11636 
11637 // Linear contribution from Higgs self-coupling
11638  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11639 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11640  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11641 
11642  // Add modifications due to small variations of the SM parameters
11643  dwidth += cHSM * ( +1. * deltaGmu()
11644  -0.789 * deltaaSMZ()
11645  +1.004 * deltaMh()
11646  +0.001 * deltamt()
11647  +1.995 * deltamc() );
11648 
11649  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11650  dwidth += eHccint + eHccpar;
11651 
11652  return dwidth;
11653 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2487
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
double eHccint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3666
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2432
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:3909
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double eHccpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3667
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHccRatio2()

double NPSMEFTd6::deltaGammaHccRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 11655 of file NPSMEFTd6.cpp.

11656 {
11657  double dwidth = 0.0;
11658 
11659 
11660  //Contributions that are quadratic in the effective coefficients
11661  return ( dwidth );
11662 
11663 }

◆ deltaGammaHgagaRatio1()

double NPSMEFTd6::deltaGammaHgagaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 11434 of file NPSMEFTd6.cpp.

11435 {
11436  double dwidth = 0.0;
11437 
11438  double C1 = 0.0049;
11439 
11440 // It does not include modifications of MW
11441 
11442 // Write the tree-level contributions directly as a function
11443 // of delta_AA (or deltaG_hAA) to account for variations of sw2 and cw2
11444 
11445  dwidth = ( -255156.97*deltaG_hAA()
11446 // -48314158. * CHB / LambdaNP2
11447 // -14510502. * CHW / LambdaNP2
11448 // +26477588. * CHWB / LambdaNP2
11449  + cLHd6 * (
11450  +119766. * CHbox / LambdaNP2
11451  -42565.7 * CeH_33r / LambdaNP2
11452  -48868.1 * CuH_22r / LambdaNP2
11453  +32078.2 * CuH_33r / LambdaNP2
11454  -18428.3 * CdH_33r / LambdaNP2
11455  -137452. * CHD / LambdaNP2
11456  -235677. * CHWB / LambdaNP2
11457  -124462. * DeltaGF() / v() / v()
11458  -1.257 * deltaMwd6() )
11459  );
11460 
11461 // Linear contribution from Higgs self-coupling
11462  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11463 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11464  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11465 
11466  // Add modifications due to small variations of the SM parameters
11467  dwidth += cHSM * ( +2. * deltaa0()
11468  +0.27 * deltaaMZ()
11469  +0.736 * deltaGmu()
11470  -1.797 * deltaMz()
11471  +0.02 * deltaaSMZ()
11472  +4.195 * deltaMh()
11473  +0.047 * deltamt()
11474  +0.008 * deltamb()
11475  +0.009 * deltamc()
11476  +0.01 * deltamtau() );
11477 
11478  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11479  dwidth += eHgagaint + eHgagapar;
11480 
11481  return dwidth;
11482 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2421
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHgagaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3660
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2487
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
virtual double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2443
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
virtual double deltaa0() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref...
Definition: NPSMEFTd6.cpp:2476
double eHgagapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3661
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
virtual double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2820
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2432
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHgagaRatio2()

double NPSMEFTd6::deltaGammaHgagaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 11484 of file NPSMEFTd6.cpp.

11485 {
11486  double dwidth = 0.0;
11487 
11488 
11489  //Contributions that are quadratic in the effective coefficients
11490  return ( dwidth );
11491 
11492 }

◆ deltaGammaHggRatio1()

double NPSMEFTd6::deltaGammaHggRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10005 of file NPSMEFTd6.cpp.

10006 {
10007  double dwidth = 0.0;
10008 
10009  double C1 = 0.0066;
10010 
10011  dwidth = ( +37526258. * CHG / LambdaNP2
10012  + cLHd6 * (
10013  +121248. * CHbox / LambdaNP2
10014  +173353. * CuH_22r / LambdaNP2
10015  -129155. * CuH_33r / LambdaNP2
10016  +248530. * CdH_33r / LambdaNP2
10017  -30312.1 * CHD / LambdaNP2
10018  -60624.1 * DeltaGF() / v() / v() )
10019  );
10020 
10021 // Linear contribution from Higgs self-coupling
10022  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10023 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10024  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10025 
10026  // Add modifications due to small variations of the SM parameters
10027  dwidth += cHSM * ( +1.003 * deltaGmu()
10028  +2.31 * deltaaSMZ()
10029  +3.276 * deltaMh()
10030  -0.134 * deltamt()
10031  -0.106 * deltamb()
10032  -0.03 * deltamc() );
10033 
10034  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10035  dwidth += eHggint + eHggpar;
10036 
10037  return dwidth;
10038 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2421
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHggpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3653
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2487
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double eHggint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3652
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2432
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHggRatio2()

double NPSMEFTd6::deltaGammaHggRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10040 of file NPSMEFTd6.cpp.

10041 {
10042  double dwidth = 0.0;
10043 
10044 
10045  //Contributions that are quadratic in the effective coefficients
10046  return ( dwidth );
10047 
10048 }

◆ deltaGammaHmumuRatio1()

double NPSMEFTd6::deltaGammaHmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 11510 of file NPSMEFTd6.cpp.

11511 {
11512  double dwidth = 0.0;
11513 
11514  double C1 = 0.0;
11515 
11516  dwidth = ( +121248. * CHbox / LambdaNP2
11517  -199792511. * CeH_22r / LambdaNP2
11518  -30312.1 * CHD / LambdaNP2
11519  -60624.1 * DeltaGF() / v() / v() );
11520 
11521 // Linear contribution from Higgs self-coupling
11522  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11523 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11524  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11525 
11526  // Add modifications due to small variations of the SM parameters
11527  dwidth += cHSM * ( +1. * deltaGmu()
11528  +1. * deltaMh() );
11529 
11530  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11531  dwidth += eHmumuint + eHmumupar;
11532 
11533  return dwidth;
11534 }
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHmumuint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3662
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double eHmumupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3663
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHmumuRatio2()

double NPSMEFTd6::deltaGammaHmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 11536 of file NPSMEFTd6.cpp.

11537 {
11538  double dwidth = 0.0;
11539 
11540 
11541  //Contributions that are quadratic in the effective coefficients
11542  return ( dwidth );
11543 
11544 }

◆ deltaGammaHtautauRatio1()

double NPSMEFTd6::deltaGammaHtautauRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 11562 of file NPSMEFTd6.cpp.

11563 {
11564  double dwidth = 0.0;
11565 
11566  double C1 = 0.0;
11567 
11568  dwidth = ( +121248. * CHbox / LambdaNP2
11569  -11880369. * CeH_33r / LambdaNP2
11570  -30312.1 * CHD / LambdaNP2
11571  -60624.1 * DeltaGF() / v() / v() );
11572 
11573 // Linear contribution from Higgs self-coupling
11574  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11575 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11576  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11577 
11578  // Add modifications due to small variations of the SM parameters
11579  dwidth += cHSM * ( +1. * deltaGmu()
11580  +1.002 * deltaMh()
11581  +1.998 * deltamtau() );
11582 
11583  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11584  dwidth += eHtautauint + eHtautaupar;
11585 
11586  return dwidth;
11587 }
double eHtautauint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3664
double eHtautaupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3665
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2443
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHtautauRatio2()

double NPSMEFTd6::deltaGammaHtautauRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 11589 of file NPSMEFTd6.cpp.

11590 {
11591  double dwidth = 0.0;
11592 
11593 
11594  //Contributions that are quadratic in the effective coefficients
11595  return ( dwidth );
11596 
11597 }

◆ deltaGammaHWffRatio1()

double NPSMEFTd6::deltaGammaHWffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 10347 of file NPSMEFTd6.cpp.

10348 {
10349  double dwidth = 0.0;
10350 
10351  double C1 = 0.0073;
10352 
10353  dwidth = ( +121288. * CHbox / LambdaNP2
10354  +5395.21 * (1.0/3.0) * ( CHL3_11 + CHL3_22 + CHL3_33 ) / LambdaNP2
10355  +11680.9 * (1.0/2.0) * ( CHQ3_11 + CHQ3_22 ) / LambdaNP2
10356  -159787. * CHD / LambdaNP2
10357  -91509.1 * CHW / LambdaNP2
10358  -283092. * CHWB / LambdaNP2
10359  +37845.1 * CDHW / LambdaNP2
10360  -3.259 * DeltaGF()
10361  -15.196 * deltaMwd6() );
10362 
10363 // Linear contribution from Higgs self-coupling
10364  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10365 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10366  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10367 
10368  // Add modifications due to small variations of the SM parameters
10369  //dwidth += cHSM * ( 0.0 );
10370 
10371  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10372  //dwidth += eHWWint + eHWWpar;
10373 
10374  return dwidth;
10375 
10376 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHWffRatio2()

double NPSMEFTd6::deltaGammaHWffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 10378 of file NPSMEFTd6.cpp.

10379 {
10380  double dwidth = 0.0;
10381 
10382 
10383  //Contributions that are quadratic in the effective coefficients
10384  return ( dwidth );
10385 
10386 }

◆ deltaGammaHWjjRatio1()

double NPSMEFTd6::deltaGammaHWjjRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10231 of file NPSMEFTd6.cpp.

10232 {
10233  double dwidth = 0.0;
10234 
10235  double C1 = 0.0073;
10236 
10237  dwidth = ( +121611. * CHbox / LambdaNP2
10238  +17701.4 * (1.0/2.0) * ( CHQ3_11 + CHQ3_22 ) / LambdaNP2
10239  -159273. * CHD / LambdaNP2
10240  -91021.6 * CHW / LambdaNP2
10241  -282574. * CHWB / LambdaNP2
10242  +37917.5 * CDHW / LambdaNP2
10243  -3.259 * DeltaGF()
10244  -15.198 * deltaMwd6() );
10245 
10246 // Linear contribution from Higgs self-coupling
10247  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10248 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10249  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10250 
10251  // Add modifications due to small variations of the SM parameters
10252  //dwidth += cHSM * ( 0.0 );
10253 
10254  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10255  //dwidth += eHWWint + eHWWpar;
10256 
10257  return dwidth;
10258 
10259 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHWjjRatio2()

double NPSMEFTd6::deltaGammaHWjjRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10261 of file NPSMEFTd6.cpp.

10262 {
10263  double dwidth = 0.0;
10264 
10265 
10266  //Contributions that are quadratic in the effective coefficients
10267  return ( dwidth );
10268 
10269 }

◆ deltaGammaHWlvRatio1()

double NPSMEFTd6::deltaGammaHWlvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10114 of file NPSMEFTd6.cpp.

10115 {
10116  double dwidth = 0.0;
10117 
10118  double C1 = 0.0073;
10119 
10120  dwidth = ( +121875. * CHbox / LambdaNP2
10121  +18351.9 * (1.0/2.0) * ( CHL3_11 + CHL3_22 ) / LambdaNP2
10122  -159873. * CHD / LambdaNP2
10123  -91288.7 * CHW / LambdaNP2
10124  -284689. * CHWB / LambdaNP2
10125  +37703.7 * CDHW / LambdaNP2
10126  -3.292 * DeltaGF()
10127  -15.14 * deltaMwd6() );
10128 
10129 // Linear contribution from Higgs self-coupling
10130  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10131 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10132  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10133 
10134  // Add modifications due to small variations of the SM parameters
10135  //dwidth += cHSM * ( 0.0 );
10136 
10137  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10138  //dwidth += eHWWint + eHWWpar;
10139 
10140  return dwidth;
10141 
10142 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHWlvRatio2()

double NPSMEFTd6::deltaGammaHWlvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10144 of file NPSMEFTd6.cpp.

10145 {
10146  double dwidth = 0.0;
10147 
10148 
10149  //Contributions that are quadratic in the effective coefficients
10150  return ( dwidth );
10151 
10152 }

◆ deltaGammaHWW2l2vRatio1()

double NPSMEFTd6::deltaGammaHWW2l2vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10170 of file NPSMEFTd6.cpp.

10171 {
10172  double dwidth = 0.0;
10173 
10174  double C1 = 0.0073;
10175 
10176  dwidth = ( +120742. * CHbox / LambdaNP2
10177  +131582. * (1.0/2.0) * ( CHL3_11 + CHL3_22 ) / LambdaNP2
10178  -204043. * CHD / LambdaNP2
10179  -91463.9 * CHW / LambdaNP2
10180  -379529. * CHWB / LambdaNP2
10181  +36848.2 * CDHW / LambdaNP2
10182  -4.705 * DeltaGF()
10183  -13.735 * deltaMwd6()
10184  -0.965 * deltaGwd6()
10185  );
10186 
10187 // Linear contribution from Higgs self-coupling
10188  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10189 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10190  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10191 
10192  // Add modifications due to small variations of the SM parameters
10193  dwidth += cHSM * ( -12.123 * deltaMz()
10194  +13.615 * deltaMh()
10195  +1.756 * deltaaMZ()
10196  +0.216 * deltaGmu() );
10197 
10198  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10199  dwidth += eHWWint + eHWWpar;
10200 
10201  return dwidth;
10202 
10203 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
virtual double deltaGwd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2576
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3654
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3655
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHWW2l2vRatio2()

double NPSMEFTd6::deltaGammaHWW2l2vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10205 of file NPSMEFTd6.cpp.

10206 {
10207  double dwidth = 0.0;
10208 
10209 
10210  //Contributions that are quadratic in the effective coefficients
10211  return ( dwidth );
10212 
10213 }

◆ deltaGammaHWW4fRatio1()

double NPSMEFTd6::deltaGammaHWW4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 10404 of file NPSMEFTd6.cpp.

10405 {
10406  double dwidth = 0.0;
10407 
10408  double C1 = 0.0073;
10409 
10410  double CWff, sf;
10411 
10412  CWff = ( CHL3_11 + CHL3_22 + CHL3_33 ) * v2_over_LambdaNP2 +
10413  Nc * ( CHQ3_11 + CHQ3_22 ) * v2_over_LambdaNP2;
10414 
10415  CWff = CWff/( 3.0 + 2.0*Nc );
10416 
10417  sf = 90362.5 * (1.0/2.0) * ( 3.0 + 2.0*Nc )/(Nc*v2) ; // Coefficient of the CWff term. From the CHQ3_11 term in the ME.
10418 
10419  dwidth = ( +121886. * CHbox / LambdaNP2
10420  + sf* CWff
10421  -204009. * CHD / LambdaNP2
10422  -91455.7 * CHW / LambdaNP2
10423  -382903. * CHWB / LambdaNP2
10424  +38314.9 * CDHW / LambdaNP2
10425  -4.757 * DeltaGF()
10426  -13.716 * deltaMwd6()
10427  -0.963 * deltaGwd6()
10428  );
10429 
10430 // Linear contribution from Higgs self-coupling
10431  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10432 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10433  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10434 
10435  // Add modifications due to small variations of the SM parameters
10436  dwidth += cHSM * ( -12.271 * deltaMz()
10437  +13.665 * deltaMh()
10438  +1.85 * deltaaMZ()
10439  +0.224 * deltaGmu() );
10440 
10441  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10442  dwidth += eHWWint + eHWWpar;
10443 
10444  return dwidth;
10445 
10446 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
virtual double deltaGwd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2576
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3654
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3655
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double Nc
The number of colours.
Definition: QCD.h:1220
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:3800
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHWW4fRatio2()

double NPSMEFTd6::deltaGammaHWW4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 10448 of file NPSMEFTd6.cpp.

10449 {
10450  double dwidth = 0.0;
10451 
10452 
10453  //Contributions that are quadratic in the effective coefficients
10454  return ( dwidth );
10455 
10456 }

◆ deltaGammaHWW4jRatio1()

double NPSMEFTd6::deltaGammaHWW4jRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10287 of file NPSMEFTd6.cpp.

10288 {
10289  double dwidth = 0.0;
10290 
10291  double C1 = 0.0073;
10292 
10293  dwidth = ( +121936. * CHbox / LambdaNP2
10294  +138860. * (1.0/2.0) * ( CHQ3_11 + CHQ3_22 ) / LambdaNP2
10295  -205023. * CHD / LambdaNP2
10296  -89938.5 * CHW / LambdaNP2
10297  -383944. * CHWB / LambdaNP2
10298  +38244.6 * CDHW / LambdaNP2
10299  -4.816 * DeltaGF()
10300  -13.647 * deltaMwd6()
10301  -0.959 * deltaGwd6() );
10302 
10303 // Linear contribution from Higgs self-coupling
10304  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10305 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10306  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10307 
10308  // Add modifications due to small variations of the SM parameters
10309  dwidth += cHSM * ( -12.168 * deltaMz()
10310  +13.66 * deltaMh()
10311  +1.899 * deltaaMZ()
10312  +0.189 * deltaGmu() );
10313 
10314  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10315  dwidth += eHWWint + eHWWpar;
10316 
10317  return dwidth;
10318 
10319 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
virtual double deltaGwd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2576
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3654
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3655
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHWW4jRatio2()

double NPSMEFTd6::deltaGammaHWW4jRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10321 of file NPSMEFTd6.cpp.

10322 {
10323  double dwidth = 0.0;
10324 
10325 
10326  //Contributions that are quadratic in the effective coefficients
10327  return ( dwidth );
10328 
10329 }

◆ deltaGammaHWWRatio1()

double NPSMEFTd6::deltaGammaHWWRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10066 of file NPSMEFTd6.cpp.

10067 {
10068  double dwidth = 0.0;
10069 
10070 // double C1 = 0.0073;
10071 
10072  dwidth = deltaGammaHWW4fRatio1();
10073 
10074 // Linear contribution from Higgs self-coupling
10075 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10076 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10077 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10078 
10079  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10080 // dwidth += eHWWint + eHWWpar;
10081 
10082  return dwidth;
10083 
10084 }
double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ deltaGammaHWWRatio2()

double NPSMEFTd6::deltaGammaHWWRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10086 of file NPSMEFTd6.cpp.

10087 {
10088  double dwidth = 0.0;
10089 
10090  //Contributions that are quadratic in the effective coefficients
10091  dwidth = deltaGammaHWW4fRatio2();
10092 
10093 
10094  return dwidth;
10095 
10096 }
double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ deltaGammaHZddRatio1()

double NPSMEFTd6::deltaGammaHZddRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 11141 of file NPSMEFTd6.cpp.

11142 {
11143  double dwidth = 0.0;
11144 
11145  double C1 = 0.0083;
11146 
11147  dwidth = ( +121756. * CHbox / LambdaNP2
11148  +9252.73 * (1.0/3.0) * ( CHQ1_11 + CHQ1_22 + CHQ1_33 ) / LambdaNP2
11149  -1471.03 * (1.0/3.0) * ( CHd_11 + CHd_22 + CHd_33 ) / LambdaNP2
11150  +9252.73 * (1.0/3.0) * ( CHQ3_11 + CHQ3_22 + CHQ3_33 ) / LambdaNP2
11151  -12714.3 * CHD / LambdaNP2
11152  -13589.3 * CHB / LambdaNP2
11153  -45689.4 * CHW / LambdaNP2
11154  -85582.3 * CHWB / LambdaNP2
11155  +17007.1 * CDHB / LambdaNP2
11156  +30733.1 * CDHW / LambdaNP2
11157  -2.427 * DeltaGF() );
11158 
11159 // Linear contribution from Higgs self-coupling
11160  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11161 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11162  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11163 
11164  // Add modifications due to small variations of the SM parameters
11165  //dwidth += cHSM * ( 0.0 );
11166 
11167  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11168  //dwidth += eHZZint + eHZZpar;
11169 
11170  return dwidth;
11171 
11172 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZddRatio2()

double NPSMEFTd6::deltaGammaHZddRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 11174 of file NPSMEFTd6.cpp.

11175 {
11176  double dwidth = 0.0;
11177 
11178 
11179  //Contributions that are quadratic in the effective coefficients
11180  return ( dwidth );
11181 
11182 }

◆ deltaGammaHZeeRatio1()

double NPSMEFTd6::deltaGammaHZeeRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 10581 of file NPSMEFTd6.cpp.

10582 {
10583  double dwidth = 0.0;
10584 
10585  double C1 = 0.0083;
10586 
10587 // Derived from the HZll expression for l=e only
10588 
10589  dwidth = ( +121715. * CHbox / LambdaNP2
10590  +8726.9 * CHL1_11 / LambdaNP2
10591  -7315.2 * CHe_11 / LambdaNP2
10592  +8726.9 * CHL3_11 / LambdaNP2
10593  -5544.15 * CHD / LambdaNP2
10594  -13560.9 * CHB / LambdaNP2
10595  -45585.2 * CHW / LambdaNP2
10596  -53507.9 * CHWB / LambdaNP2
10597  +16829.2 * CDHB / LambdaNP2
10598  +30766.6 * CDHW / LambdaNP2
10599  -2.204 * DeltaGF() );
10600 
10601 // Linear contribution from Higgs self-coupling
10602  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10603 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10604  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10605 
10606  // Add modifications due to small variations of the SM parameters
10607  //dwidth += cHSM * ( 0.0 );
10608 
10609  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10610  //dwidth += eHZZint + eHZZpar;
10611 
10612  return dwidth;
10613 
10614 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZeeRatio2()

double NPSMEFTd6::deltaGammaHZeeRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 10616 of file NPSMEFTd6.cpp.

10617 {
10618  double dwidth = 0.0;
10619 
10620 
10621  //Contributions that are quadratic in the effective coefficients
10622  return ( dwidth );
10623 
10624 }

◆ deltaGammaHZffRatio1()

double NPSMEFTd6::deltaGammaHZffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 11200 of file NPSMEFTd6.cpp.

11201 {
11202  double dwidth = 0.0;
11203 
11204  double C1 = 0.0083;
11205 
11206  dwidth = ( +121551. * CHbox / LambdaNP2
11207  -824.482 * (1.0/3.0) * ( CHL1_11 + CHL1_22 + CHL1_33 ) / LambdaNP2
11208  +1840.54 * (1.0/12.0) * ( 5.0 * CHQ1_11 + 5.0 * CHQ1_22 + 2.0 * CHQ1_33 - CHQ3_11 - CHQ3_22 + 2.0 * CHQ3_33 ) / LambdaNP2
11209  -795.383 * (1.0/3.0) * ( CHe_11 + CHe_22 + CHe_33 ) / LambdaNP2
11210  +1069.4 * (1.0/2.0) * ( CHu_11 + CHu_22 ) / LambdaNP2
11211  -579.563 * (1.0/3.0) * ( CHd_11 + CHd_22 + CHd_33 ) / LambdaNP2
11212  +3164.56 * (1.0/3.0) * ( CHL3_11 + CHL3_22 + CHL3_33 ) / LambdaNP2
11213  +6413.99 * (-1.0/12.0) * ( CHQ1_11 + CHQ1_22 - 2.0 * CHQ1_33 - 5.0 * CHQ3_11 - 5.0 * CHQ3_22 - 2.0 * CHQ3_33) / LambdaNP2
11214  -10839.5 * CHD / LambdaNP2
11215  -14222.3 * CHB / LambdaNP2
11216  -45455.6 * CHW / LambdaNP2
11217  -75343.1 * CHWB / LambdaNP2
11218  +16804.9 * CDHB / LambdaNP2
11219  +30421. * CDHW / LambdaNP2
11220  -2.356 * DeltaGF() );
11221 
11222 // Linear contribution from Higgs self-coupling
11223  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11224 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11225  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11226 
11227  // Add modifications due to small variations of the SM parameters
11228  //dwidth += cHSM * ( 0.0 );
11229 
11230  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11231  //dwidth += eHZZint + eHZZpar;
11232 
11233  return dwidth;
11234 
11235 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZffRatio2()

double NPSMEFTd6::deltaGammaHZffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 11237 of file NPSMEFTd6.cpp.

11238 {
11239  double dwidth = 0.0;
11240 
11241 
11242  //Contributions that are quadratic in the effective coefficients
11243  return ( dwidth );
11244 
11245 }

◆ deltaGammaHZgaRatio1()

double NPSMEFTd6::deltaGammaHZgaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 11349 of file NPSMEFTd6.cpp.

11350 {
11351  double dwidth = 0.0;
11352 
11353  double C1 = 0.0;
11354 
11355 // It includes modifications of Zff vertices and MW, but not on the pure VVV and VVVV vertices
11356 
11357 // Write the tree-level contributions directly as a function
11358 // of delta_ZA (or deltaG1_hZA()) to account for variations of sw2 and cw2
11359 
11360  dwidth = ( -71769.02 * deltaG1_hZA()
11361 // +14894914. * CHB / LambdaNP2
11362 // -14894913. * CHW / LambdaNP2
11363 // +9508089. * CHWB / LambdaNP2
11364 // -2869576. * CDHB / LambdaNP2
11365 // +1572613. * CDHW / LambdaNP2
11366  + cLHd6 * (
11367  +120002. * CHbox / LambdaNP2
11368  +50.12 * CHL1_33 / LambdaNP2
11369  +17401. * CHQ1_33 / LambdaNP2
11370  +50.12 * CHe_33 / LambdaNP2
11371  +17188.7 * CHu_33 / LambdaNP2
11372  +212.376 * CHd_33 / LambdaNP2
11373  +50.12 * CHL3_33 / LambdaNP2
11374  -16976.3 * CHQ3_33 / LambdaNP2
11375  -373.856 * CeH_33r / LambdaNP2
11376  -2953.05 * CuH_22r / LambdaNP2
11377  +6636.34 * CuH_33r / LambdaNP2
11378  -6121.66 * CdH_33r / LambdaNP2
11379  -111254. * CHD / LambdaNP2
11380  -162538. * CHWB / LambdaNP2
11381  -96076.1 * DeltaGF() / v() / v()
11382  -0.123 * deltaMwd6() )
11383  );
11384 
11385 // Linear contribution from Higgs self-coupling
11386  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11387 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11388  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11389 
11390  // Add modifications due to small variations of the SM parameters
11391  dwidth += cHSM * ( +1. * deltaa0()
11392  -0.629 * deltaaMZ()
11393  +2.629 * deltaGmu()
11394  -4.926 * deltaMz()
11395  +0.004 * deltaaSMZ()
11396  +11.167 * deltaMh()
11397  +0.013 * deltamt()
11398  +0.004 * deltamb()
11399  +0.001 * deltamc()
11400  +0. * deltamtau() );
11401 
11402  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11403  dwidth += eHZgaint + eHZgapar;
11404 
11405  return dwidth;
11406 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2421
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3494
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eHZgaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3658
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2487
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double eHZgapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3659
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
virtual double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2443
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
virtual double deltaa0() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref...
Definition: NPSMEFTd6.cpp:2476
virtual double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2730
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2432
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZgaRatio2()

double NPSMEFTd6::deltaGammaHZgaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 11408 of file NPSMEFTd6.cpp.

11409 {
11410  double dwidth = 0.0;
11411 
11412 
11413  //Contributions that are quadratic in the effective coefficients
11414  return ( dwidth );
11415 
11416 }

◆ deltaGammaHZllRatio1()

double NPSMEFTd6::deltaGammaHZllRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 10522 of file NPSMEFTd6.cpp.

10523 {
10524  double dwidth = 0.0;
10525 
10526  double C1 = 0.0083;
10527 
10528  dwidth = ( +121715. * CHbox / LambdaNP2
10529  +8726.9 * (1.0/2.0) * ( CHL1_11 + CHL1_22 ) / LambdaNP2
10530  -7315.2 * (1.0/2.0) * ( CHe_11 + CHe_22 ) / LambdaNP2
10531  +8726.9 * (1.0/2.0) * ( CHL3_11 + CHL3_22 ) / LambdaNP2
10532  -5544.15 * CHD / LambdaNP2
10533  -13560.9 * CHB / LambdaNP2
10534  -45585.2 * CHW / LambdaNP2
10535  -53507.9 * CHWB / LambdaNP2
10536  +16829.2 * CDHB / LambdaNP2
10537  +30766.6 * CDHW / LambdaNP2
10538  -2.204 * DeltaGF() );
10539 
10540 // Linear contribution from Higgs self-coupling
10541  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10542 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10543  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10544 
10545  // Add modifications due to small variations of the SM parameters
10546  //dwidth += cHSM * ( 0.0 );
10547 
10548  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10549  //dwidth += eHZZint + eHZZpar;
10550 
10551  return dwidth;
10552 
10553 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZllRatio2()

double NPSMEFTd6::deltaGammaHZllRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 10555 of file NPSMEFTd6.cpp.

10556 {
10557  double dwidth = 0.0;
10558 
10559 
10560  //Contributions that are quadratic in the effective coefficients
10561  return ( dwidth );
10562 
10563 }

◆ deltaGammaHZmumuRatio1()

double NPSMEFTd6::deltaGammaHZmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 10642 of file NPSMEFTd6.cpp.

10643 {
10644  double dwidth = 0.0;
10645 
10646  double C1 = 0.0083;
10647 
10648 // Derived from the HZll expression for l=mu only
10649 
10650  dwidth = ( +121715. * CHbox / LambdaNP2
10651  +8726.9 * CHL1_22 / LambdaNP2
10652  -7315.2 * CHe_22 / LambdaNP2
10653  +8726.9 * CHL3_22 / LambdaNP2
10654  -5544.15 * CHD / LambdaNP2
10655  -13560.9 * CHB / LambdaNP2
10656  -45585.2 * CHW / LambdaNP2
10657  -53507.9 * CHWB / LambdaNP2
10658  +16829.2 * CDHB / LambdaNP2
10659  +30766.6 * CDHW / LambdaNP2
10660  -2.204 * DeltaGF() );
10661 
10662 // Linear contribution from Higgs self-coupling
10663  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10664 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10665  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10666 
10667  // Add modifications due to small variations of the SM parameters
10668  //dwidth += cHSM * ( 0.0 );
10669 
10670  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10671  //dwidth += eHZZint + eHZZpar;
10672 
10673  return dwidth;
10674 
10675 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZmumuRatio2()

double NPSMEFTd6::deltaGammaHZmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 10677 of file NPSMEFTd6.cpp.

10678 {
10679  double dwidth = 0.0;
10680 
10681 
10682  //Contributions that are quadratic in the effective coefficients
10683  return ( dwidth );
10684 
10685 }

◆ deltaGammaHZuuRatio1()

double NPSMEFTd6::deltaGammaHZuuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 11082 of file NPSMEFTd6.cpp.

11083 {
11084  double dwidth = 0.0;
11085 
11086  double C1 = 0.0083;
11087 
11088  dwidth = ( +121512. * CHbox / LambdaNP2
11089  -9648.28 * (1.0/2.0) * ( CHQ1_11 + CHQ1_22 ) / LambdaNP2
11090  +4218.6 * (1.0/2.0) * ( CHu_11 + CHu_22 ) / LambdaNP2
11091  +9648.28 * (1.0/2.0) * ( CHQ3_11 + CHQ3_22 ) / LambdaNP2
11092  -17762.5 * CHD / LambdaNP2
11093  -13473.3 * CHB / LambdaNP2
11094  -45667.9 * CHW / LambdaNP2
11095  -110057. * CHWB / LambdaNP2
11096  +16854.2 * CDHB / LambdaNP2
11097  +30781.7 * CDHW / LambdaNP2
11098  -2.6 * DeltaGF() );
11099 
11100 // Linear contribution from Higgs self-coupling
11101  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11102 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11103  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11104 
11105  // Add modifications due to small variations of the SM parameters
11106  //dwidth += cHSM * ( 0.0 );
11107 
11108  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11109  //dwidth += eHZZint + eHZZpar;
11110 
11111  return dwidth;
11112 
11113 }
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZuuRatio2()

double NPSMEFTd6::deltaGammaHZuuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 11115 of file NPSMEFTd6.cpp.

11116 {
11117  double dwidth = 0.0;
11118 
11119 
11120  //Contributions that are quadratic in the effective coefficients
11121  return ( dwidth );
11122 
11123 }

◆ deltaGammaHZvvRatio1()

double NPSMEFTd6::deltaGammaHZvvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 10961 of file NPSMEFTd6.cpp.

10962 {
10963  double dwidth = 0.0;
10964 
10965  double C1 = 0.0083;
10966 
10967  dwidth = ( +121530. * CHbox / LambdaNP2
10968  -7943.34 * (1.0/3.0) * ( CHL1_11 + CHL1_22 + CHL1_33 ) / LambdaNP2
10969  +7943.34 * (1.0/3.0) * ( CHL3_11 + CHL3_22 + CHL3_33 ) / LambdaNP2
10970  -229.41 * CHD / LambdaNP2
10971  -13535.2 * CHB / LambdaNP2
10972  -45480.6 * CHW / LambdaNP2
10973  -24891. * CHWB / LambdaNP2
10974  +16833. * CDHB / LambdaNP2
10975  +30597.6 * CDHW / LambdaNP2
10976  -2. * DeltaGF() );
10977 
10978 // Linear contribution from Higgs self-coupling
10979  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10980 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10981  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10982 
10983  // Add modifications due to small variations of the SM parameters
10984  //dwidth += cHSM * ( 0.0 );
10985 
10986  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10987  //dwidth += eHZZint + eHZZpar;
10988 
10989  return dwidth;
10990 
10991 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ deltaGammaHZvvRatio2()

double NPSMEFTd6::deltaGammaHZvvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 10993 of file NPSMEFTd6.cpp.

10994 {
10995  double dwidth = 0.0;
10996 
10997 
10998  //Contributions that are quadratic in the effective coefficients
10999  return ( dwidth );
11000 
11001 }

◆ deltaGammaHZZ2e2muRatio1()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 10836 of file NPSMEFTd6.cpp.

10837 {
10838  double dwidth = 0.0;
10839 
10840  double C1 = 0.0083;
10841 
10842  dwidth = ( +120836. * CHbox / LambdaNP2
10843  +126374. * (1.0/2.0) * ( CHL1_11 + CHL1_22 ) / LambdaNP2
10844  -109064. * (1.0/2.0) * ( CHe_11 + CHe_22 ) / LambdaNP2
10845  +126374. * (1.0/2.0) * ( CHL3_11 + CHL3_22 ) / LambdaNP2
10846  -42370.4 * CHD / LambdaNP2
10847  -14299. * CHB / LambdaNP2
10848  -47298.2 * CHW / LambdaNP2
10849  -83098.2 * CHWB / LambdaNP2
10850  +16362.7 * CDHB / LambdaNP2
10851  +29503.4 * CDHW / LambdaNP2
10852  -3.378 * DeltaGF()
10853  -0.85 * deltaGzd6() );
10854 
10855 // Linear contribution from Higgs self-coupling
10856  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10857 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10858  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10859 
10860  // Add modifications due to small variations of the SM parameters
10861  dwidth += cHSM * ( -10.07 * deltaMz()
10862  +15.626 * deltaMh()
10863  -0.128 * deltaaMZ()
10864  +2.258 * deltaGmu() );
10865 
10866  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10867  dwidth += eHZZint + eHZZpar;
10868 
10869  return dwidth;
10870 
10871 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ2e2muRatio2()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 10873 of file NPSMEFTd6.cpp.

10874 {
10875  double dwidth = 0.0;
10876 
10877  //Contributions that are quadratic in the effective coefficients
10878  return ( dwidth );
10879 
10880 }

◆ deltaGammaHZZ4dRatio1()

double NPSMEFTd6::deltaGammaHZZ4dRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2361 of file NPSMEFTd6.h.

2362  {
2363  return 1.0;
2364  };

◆ deltaGammaHZZ4dRatio2()

double NPSMEFTd6::deltaGammaHZZ4dRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4eRatio1()

double NPSMEFTd6::deltaGammaHZZ4eRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 10773 of file NPSMEFTd6.cpp.

10774 {
10775  double dwidth = 0.0;
10776 
10777  double C1 = 0.0083;
10778 
10779  dwidth = ( +121386. * CHbox / LambdaNP2
10780  +123413. * CHL1_11 / LambdaNP2
10781  -103717. * CHe_11 / LambdaNP2
10782  +123413. * CHL3_11 / LambdaNP2
10783  -44056.9 * CHD / LambdaNP2
10784  -13385.3 * CHB / LambdaNP2
10785  -45127.7 * CHW / LambdaNP2
10786  -91708.7 * CHWB / LambdaNP2
10787  +16138.9 * CDHB / LambdaNP2
10788  +28759.4 * CDHW / LambdaNP2
10789  -3.462 * DeltaGF()
10790  -0.769 * deltaGzd6() );
10791 
10792 // Linear contribution from Higgs self-coupling
10793  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10794 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10795  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10796 
10797  // Add modifications due to small variations of the SM parameters
10798  dwidth += cHSM * ( -9.228 * deltaMz()
10799  +15.148 * deltaMh()
10800  -0.229 * deltaaMZ()
10801  +2.493 * deltaGmu() );
10802 
10803  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10804  dwidth += eHZZint + eHZZpar;
10805 
10806  return dwidth;
10807 
10808 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ4eRatio2()

double NPSMEFTd6::deltaGammaHZZ4eRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 10810 of file NPSMEFTd6.cpp.

10811 {
10812  double dwidth = 0.0;
10813 
10814 
10815  //Contributions that are quadratic in the effective coefficients
10816  return ( dwidth );
10817 
10818 }

◆ deltaGammaHZZ4fRatio1()

double NPSMEFTd6::deltaGammaHZZ4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11263 of file NPSMEFTd6.cpp.

11264 {
11265  double dwidth = 0.0;
11266 
11267  double C1 = 0.0083;
11268 
11269  double CZff, sf;
11270 
11271  CZff = gZvL*(-0.5 * (CHL1_11 + CHL1_22 + CHL1_33 - CHL3_11 - CHL3_22 - CHL3_33) * v2_over_LambdaNP2) +
11273  gZlR*(-0.5 * (CHe_11 + CHe_22 + CHe_33) * v2_over_LambdaNP2) +
11274  Nc * (
11276  gZdR*(-0.5 * (CHd_11 + CHd_22 + CHd_33) * v2_over_LambdaNP2) +
11277  gZuL*(-0.5 * (CHQ1_11 + CHQ1_22 - CHQ3_11 - CHQ3_22) * v2_over_LambdaNP2) +
11278  gZuR*(-0.5 * (CHu_11 + CHu_22) * v2_over_LambdaNP2)
11279  );
11280 
11281  CZff = CZff/(
11282  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
11283  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
11284  );
11285 
11286  sf = -11267.6 * (1.0/3.0) * (
11287  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
11288  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
11289  );
11290 
11291  sf = sf/(-0.5*(gZlL + gZvL)*v2) ; // Coefficient of the CZff term. From the CHL1_11 term in the ME.
11292 
11293  dwidth = ( +121373. * CHbox / LambdaNP2
11294  + sf*CZff
11295  -50927.1 * CHD / LambdaNP2
11296  -14137.9 * CHB / LambdaNP2
11297  -46350.1 * CHW / LambdaNP2
11298  -126336. * CHWB / LambdaNP2
11299  +16558.7 * CDHB / LambdaNP2
11300  +29628.7 * CDHW / LambdaNP2
11301  -3.715 * DeltaGF()
11302  -0.834 * deltaGzd6()
11303  );
11304 
11305 // Linear contribution from Higgs self-coupling
11306  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11307 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11308  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11309 
11310  // Add modifications due to small variations of the SM parameters
11311  dwidth += cHSM * ( -9.548 * deltaMz()
11312  +15.799 * deltaMh()
11313  -0.412 * deltaaMZ()
11314  +2.569 * deltaGmu() );
11315 
11316  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11317  dwidth += eHZZint + eHZZpar;
11318 
11319  return dwidth;
11320 
11321 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double gZdR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3816
double gZuL
Definition: NPSMEFTd6.h:3815
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double gZlL
Definition: NPSMEFTd6.h:3814
double gZvL
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3813
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
double Nc
The number of colours.
Definition: QCD.h:1220
double gZlR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3814
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double gZuR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3815
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double gZdL
Definition: NPSMEFTd6.h:3816
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:3800
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ4fRatio2()

double NPSMEFTd6::deltaGammaHZZ4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11323 of file NPSMEFTd6.cpp.

11324 {
11325  double dwidth = 0.0;
11326 
11327 
11328  //Contributions that are quadratic in the effective coefficients
11329  return ( dwidth );
11330 
11331 }

◆ deltaGammaHZZ4lRatio1()

double NPSMEFTd6::deltaGammaHZZ4lRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 10703 of file NPSMEFTd6.cpp.

10704 {
10705  double dwidth = 0.0;
10706 
10707  double C1 = 0.0083;
10708 
10709  double CZll, sf;
10710 
10711  CZll = gZlL*(-0.5 * (CHL1_11 + CHL1_22 + CHL3_11 + CHL3_22) * v2_over_LambdaNP2) +
10712  gZlR*(-0.5 * (CHe_11 + CHe_22) * v2_over_LambdaNP2);
10713 
10714  CZll = CZll/(2.0*(gZlL*gZlL + gZlR*gZlR));
10715 
10716  sf = 124479. * (1.0/2.0) * (2.0*(gZlL*gZlL + gZlR*gZlR))/(-0.5*gZlL*v2) ; // Coefficient of the CZll term. From the CHL1_11 term in the ME.
10717 
10718  dwidth = ( +122273. * CHbox / LambdaNP2
10719  + sf*CZll
10720  -44025.7 * CHD / LambdaNP2
10721  -13602.6 * CHB / LambdaNP2
10722  -45248.6 * CHW / LambdaNP2
10723  -88372.1 * CHWB / LambdaNP2
10724  +16088.6 * CDHB / LambdaNP2
10725  +29210.1 * CDHW / LambdaNP2
10726  -3.462 * DeltaGF()
10727  -0.808 * deltaGzd6() );
10728 
10729 // Linear contribution from Higgs self-coupling
10730  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10731 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10732  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10733 
10734  // Add modifications due to small variations of the SM parameters
10735  dwidth += cHSM * ( -9.734 * deltaMz()
10736  +15.37 * deltaMh()
10737  -0.154 * deltaaMZ()
10738  +2.339 * deltaGmu() );
10739 
10740  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10741  dwidth += eHZZint + eHZZpar;
10742 
10743  return dwidth;
10744 
10745 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double gZlL
Definition: NPSMEFTd6.h:3814
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
double gZlR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3814
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:3800
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ4lRatio2()

double NPSMEFTd6::deltaGammaHZZ4lRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 10747 of file NPSMEFTd6.cpp.

10748 {
10749  double dwidth = 0.0;
10750 
10751 
10752  //Contributions that are quadratic in the effective coefficients
10753  return ( dwidth );
10754 
10755 }

◆ deltaGammaHZZ4muRatio1()

double NPSMEFTd6::deltaGammaHZZ4muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 10898 of file NPSMEFTd6.cpp.

10899 {
10900  double dwidth = 0.0;
10901 
10902  double C1 = 0.0083;
10903 
10904  dwidth = ( +120688. * CHbox / LambdaNP2
10905  +123059. * CHL1_22 / LambdaNP2
10906  -103862. * CHe_22 / LambdaNP2
10907  +123059. * CHL3_22 / LambdaNP2
10908  -43977.1 * CHD / LambdaNP2
10909  -13575.5 * CHB / LambdaNP2
10910  -45200.8 * CHW / LambdaNP2
10911  -91625.2 * CHWB / LambdaNP2
10912  +15449.3 * CDHB / LambdaNP2
10913  +28489.5 * CDHW / LambdaNP2
10914  -3.471 * DeltaGF()
10915  -0.774 * deltaGzd6() );
10916 
10917 // Linear contribution from Higgs self-coupling
10918  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10919 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10920  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10921 
10922  // Add modifications due to small variations of the SM parameters
10923  dwidth += cHSM * ( -9.254 * deltaMz()
10924  +15.109 * deltaMh()
10925  -0.207 * deltaaMZ()
10926  +2.405 * deltaGmu() );
10927 
10928  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10929  dwidth += eHZZint + eHZZpar;
10930 
10931  return dwidth;
10932 
10933 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ4muRatio2()

double NPSMEFTd6::deltaGammaHZZ4muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 10935 of file NPSMEFTd6.cpp.

10936 {
10937  double dwidth = 0.0;
10938 
10939 
10940  //Contributions that are quadratic in the effective coefficients
10941  return ( dwidth );
10942 
10943 }

◆ deltaGammaHZZ4uRatio1()

double NPSMEFTd6::deltaGammaHZZ4uRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 2344 of file NPSMEFTd6.h.

2345  {
2346  return 1.0;
2347  };

◆ deltaGammaHZZ4uRatio2()

double NPSMEFTd6::deltaGammaHZZ4uRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4vRatio1()

double NPSMEFTd6::deltaGammaHZZ4vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11019 of file NPSMEFTd6.cpp.

11020 {
11021  double dwidth = 0.0;
11022 
11023  double C1 = 0.0083;
11024 
11025  dwidth = ( +120596. * CHbox / LambdaNP2
11026  -115532. * (1.0/3.0) * ( CHL1_11 + CHL1_22 + CHL1_33 ) / LambdaNP2
11027  +115532. * (1.0/3.0) * ( CHL3_11 + CHL3_22 + CHL3_33 ) / LambdaNP2
11028  -28744.1 * CHD / LambdaNP2
11029  -13816.7 * CHB / LambdaNP2
11030  -44782.1 * CHW / LambdaNP2
11031  -25256.6 * CHWB / LambdaNP2
11032  +15982.5 * CDHB / LambdaNP2
11033  +28910.7 * CDHW / LambdaNP2
11034  -3.013 * DeltaGF()
11035  -0.787 * deltaGzd6()
11036  );
11037 
11038 // Linear contribution from Higgs self-coupling
11039  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11040 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11041  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11042 
11043  // Add modifications due to small variations of the SM parameters
11044  dwidth += cHSM * ( -10.49 * deltaMz()
11045  +15.294 * deltaMh()
11046  +0.255 * deltaaMZ()
11047  +1.979 * deltaGmu() );
11048 
11049  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11050  dwidth += eHZZint + eHZZpar;
11051 
11052  return dwidth;
11053 
11054 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:2588
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ deltaGammaHZZ4vRatio2()

double NPSMEFTd6::deltaGammaHZZ4vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11056 of file NPSMEFTd6.cpp.

11057 {
11058  double dwidth = 0.0;
11059 
11060 
11061  //Contributions that are quadratic in the effective coefficients
11062  return ( dwidth );
11063 
11064 }

◆ deltaGammaHZZRatio1()

double NPSMEFTd6::deltaGammaHZZRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 10474 of file NPSMEFTd6.cpp.

10475 {
10476  double dwidth = 0.0;
10477 
10478 // double C1 = 0.0083;
10479 
10480  dwidth = deltaGammaHZZ4fRatio1();
10481 
10482 // Linear contribution from Higgs self-coupling
10483 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10484 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10485 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
10486 
10487  // SM (1) + intrinsic + parametric theory relative errors (free pars)
10488 // dwidth += eHZZint + eHZZpar;
10489 
10490  return dwidth;
10491 
10492 }
double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ deltaGammaHZZRatio2()

double NPSMEFTd6::deltaGammaHZZRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 10494 of file NPSMEFTd6.cpp.

10495 {
10496  double dwidth = 0.0;
10497 
10498  //Contributions that are quadratic in the effective coefficients
10499  dwidth = deltaGammaHZZ4fRatio2();
10500 
10501 
10502  return dwidth;
10503 
10504 }
double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ deltaGammaTotalRatio1()

double NPSMEFTd6::deltaGammaTotalRatio1 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 9948 of file NPSMEFTd6.cpp.

9949 {
9950  double deltaGammaRatio;
9951 
9952 // The change in the ratio asumming only SM decays
9953  deltaGammaRatio = ( trueSM.computeBrHtogg() * deltaGammaHggRatio1()
9962 
9963 // Add the effect of the invisible and exotic BR. Include also here the
9964 // pure contribution from BrHinv and BrHexo even in case of no dim 6 contibutions
9965  deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
9966 
9967  return deltaGammaRatio;
9968 }
double computeBrHtocc() const
The Br in the Standard Model.
double computeBrHtoZga() const
The Br in the Standard Model.
StandardModel trueSM
Definition: NPbase.h:1902
double computeBrHtoWW() const
The Br in the Standard Model.
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtomumu() const
The Br in the Standard Model.
double computeBrHtoZZ() const
The Br in the Standard Model.
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtotautau() const
The Br in the Standard Model.
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794
double computeBrHtogg() const
The Br in the Standard Model.
double computeBrHtogaga() const
The Br in the Standard Model.
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:3793
double computeBrHtobb() const
The Br in the Standard Model.
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ deltaGammaTotalRatio2()

double NPSMEFTd6::deltaGammaTotalRatio2 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 9970 of file NPSMEFTd6.cpp.

9971 {
9972  double deltaGammaRatio;
9973 
9974 // The change in the ratio asumming only SM decays
9975  deltaGammaRatio = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
9984 
9985 // Add the effect of the invisible and exotic BR and return
9986  return (deltaGammaRatio / (1.0 - BrHinv - BrHexo));
9987 }
double computeBrHtocc() const
The Br in the Standard Model.
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtoZga() const
The Br in the Standard Model.
StandardModel trueSM
Definition: NPbase.h:1902
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtoWW() const
The Br in the Standard Model.
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtomumu() const
The Br in the Standard Model.
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtoZZ() const
The Br in the Standard Model.
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double computeBrHtotautau() const
The Br in the Standard Model.
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794
double computeBrHtogg() const
The Br in the Standard Model.
double computeBrHtogaga() const
The Br in the Standard Model.
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:3793
double computeBrHtobb() const
The Br in the Standard Model.
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ DeltaGF()

double NPSMEFTd6::DeltaGF ( ) const
virtual

New physics contribution to the Fermi constant.

The new physics contribution \(\Delta G\) is defined as

\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]

where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.

Returns
\(\Delta G\)

Reimplemented from NPbase.

Definition at line 2356 of file NPSMEFTd6.cpp.

2357 {
2358  return ((CHL3_11 + CHL3_22 - 0.5 * (CLL_1221 + CLL_2112)) * v2_over_LambdaNP2);
2359 }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CLL_1221
Definition: NPSMEFTd6.h:3592
double CLL_2112
Definition: NPSMEFTd6.h:3592
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ deltaGL_f()

double NPSMEFTd6::deltaGL_f ( const Particle  p) const

New physics contribution to the neutral-current left-handed coupling \(g_L^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_L^f\)

Definition at line 2610 of file NPSMEFTd6.cpp.

2611 {
2612  double I3p = p.getIsospin(), Qp = p.getCharge();
2613  double CHF1 = CHF1_diag(p);
2614  double CHF3 = CHF3_diag(p);
2615  double NPindirect;
2616 
2617  NPindirect = -I3p / 4.0 * (CHD * v2_over_LambdaNP2 + 2.0 * DeltaGF())
2618  - Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
2619  *((4.0 * cW_tree / sW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2620 
2621  double NPdirect = -0.5 * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2;
2622  return (NPindirect + NPdirect);
2623 }
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
double CHF1_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2172
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2190

◆ deltaGL_Wff()

gslpp::complex NPSMEFTd6::deltaGL_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{L}\)

Reimplemented from NPbase.

Definition at line 2641 of file NPSMEFTd6.cpp.

2642 {
2643  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2644  throw std::runtime_error("NPSMEFTd6::deltaGL_Wff(): Not implemented");
2645 
2646  double CHF3 = CHF3_diag(pbar);
2647  double NPindirect;
2648 
2649  NPindirect = -cW2_tree / 4.0 / (cW2_tree - sW2_tree)
2650  * ((4.0 * sW_tree / cW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2651 
2652  double NPdirect = CHF3 * v2_over_LambdaNP2;
2653  return (NPindirect + NPdirect);
2654 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
int getIndex() const
Definition: Particle.h:160
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2190

◆ deltaGL_Wffh()

gslpp::complex NPSMEFTd6::deltaGL_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{L}\)

Definition at line 2901 of file NPSMEFTd6.cpp.

2902 {
2903  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2904  throw std::runtime_error("NPSMEFTd6::deltaGL_Wffh(): Not implemented");
2905 
2906  double CHF3 = CHF3_diag(pbar);
2907  return (2.0 * sqrt(2.0) * Mz * cW_tree / v() / v() * CHF3 * v2_over_LambdaNP2);
2908 }
double Mz
The mass of the boson in GeV.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
int getIndex() const
Definition: Particle.h:160
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2190
complex sqrt(const complex &z)

◆ deltaGL_Zffh()

double NPSMEFTd6::deltaGL_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{L}\)

Definition at line 2919 of file NPSMEFTd6.cpp.

2920 {
2921  double I3p = p.getIsospin();
2922  double CHF1 = CHF1_diag(p);
2923  double CHF3 = CHF3_diag(p);
2924  return (-2.0 * Mz / v() / v() * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2);
2925 }
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
double CHF1_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2172
double Mz
The mass of the boson in GeV.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F...
Definition: NPSMEFTd6.cpp:2190

◆ deltaGmu()

double NPSMEFTd6::deltaGmu ( ) const
virtual

The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta G_\mu/G_\mu\)

Definition at line 2454 of file NPSMEFTd6.cpp.

2455 {
2456  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2457  return ( (GF - 1.1663787/100000.0 ) / (1.1663787/100000.0) );
2458 }
double GF
The Fermi constant in .

◆ deltaGmu2()

double NPSMEFTd6::deltaGmu2 ( ) const
virtual

The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta G_\mu/G_\mu)^2\)

Definition at line 2460 of file NPSMEFTd6.cpp.

2461 {
2462  return ( 0.0 );
2463 }

◆ deltaGR_f()

double NPSMEFTd6::deltaGR_f ( const Particle  p) const

New physics contribution to the neutral-current right-handed coupling \(g_R^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_R^f\)

Definition at line 2625 of file NPSMEFTd6.cpp.

2626 {
2627  double Qp = p.getCharge();
2628  double CHf = CHf_diag(p);
2629  double NPindirect;
2630 
2631  NPindirect = -Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
2632  *((4.0 * cW_tree / sW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
2633 
2634  double NPdirect = -0.5 * CHf*v2_over_LambdaNP2;
2635  return (NPindirect + NPdirect);
2636 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double CHf_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f...
Definition: NPSMEFTd6.cpp:2208
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440

◆ deltaGR_Wff()

gslpp::complex NPSMEFTd6::deltaGR_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{R}\)

Reimplemented from NPbase.

Definition at line 2656 of file NPSMEFTd6.cpp.

2657 {
2658  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2659  throw std::runtime_error("NPSMEFTd6::deltaGR_Wff(): Not implemented");
2660 
2661  gslpp::complex CHud = CHud_diag(pbar);
2662  return (0.5 * CHud * v2_over_LambdaNP2);
2663 }
gslpp::complex CHud_diag(const Particle u) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f...
Definition: NPSMEFTd6.cpp:2234
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
int getIndex() const
Definition: Particle.h:160
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35

◆ deltaGR_Wffh()

gslpp::complex NPSMEFTd6::deltaGR_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{R}\)

Definition at line 2910 of file NPSMEFTd6.cpp.

2911 {
2912  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
2913  throw std::runtime_error("NPSMEFTd6::deltaGR_Wffh(): Not implemented");
2914 
2915  gslpp::complex CHud = CHud_diag(pbar);
2916  return (sqrt(2.0) * Mz * cW_tree / v() / v() * CHud * v2_over_LambdaNP2);
2917 }
double Mz
The mass of the boson in GeV.
gslpp::complex CHud_diag(const Particle u) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f...
Definition: NPSMEFTd6.cpp:2234
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
int getIndex() const
Definition: Particle.h:160
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
complex sqrt(const complex &z)

◆ deltaGR_Zffh()

double NPSMEFTd6::deltaGR_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{R}\)

Definition at line 2927 of file NPSMEFTd6.cpp.

2928 {
2929  double CHf = CHf_diag(p);
2930  return (-2.0 * Mz / v() / v() * CHf * v2_over_LambdaNP2);
2931 }
double Mz
The mass of the boson in GeV.
double CHf_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f...
Definition: NPSMEFTd6.cpp:2208
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...

◆ deltaGV_f()

double NPSMEFTd6::deltaGV_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current vector coupling \(g_V^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_V^f\)

Reimplemented from NPbase.

Definition at line 2600 of file NPSMEFTd6.cpp.

2601 {
2602  return (deltaGL_f(p) + deltaGR_f(p));
2603 }
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPSMEFTd6.cpp:2610
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPSMEFTd6.cpp:2625

◆ deltaGwd6()

double NPSMEFTd6::deltaGwd6 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).

Returns
\(\delta \Gamma_W/\Gamma_W\)

Definition at line 2576 of file NPSMEFTd6.cpp.

2577 {
2578  return ( deltaGamma_W() / trueSM.GammaW() );
2579 }
StandardModel trueSM
Definition: NPbase.h:1902
virtual double deltaGamma_W() const
The new physics contribution to the total decay width of the boson, .
Definition: NPSMEFTd6.cpp:2558
virtual double GammaW(const Particle fi, const Particle fj) const
A partial decay width of the boson decay into a SM fermion pair.

◆ deltaGwd62()

double NPSMEFTd6::deltaGwd62 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).

Returns
\((\delta \Gamma_W/\Gamma_W)^2\)

Definition at line 2581 of file NPSMEFTd6.cpp.

2582 {
2583  double dWW = 0.0;
2584 
2585  return (dWW*dWW);
2586 }

◆ deltaGzd6()

double NPSMEFTd6::deltaGzd6 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).

Returns
\(\delta \Gamma_Z/\Gamma_Z\)

Definition at line 2588 of file NPSMEFTd6.cpp.

2589 {
2590  return ( deltaGamma_Z() / trueSM.Gamma_Z() );
2591 }
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176

◆ deltaGzd62()

double NPSMEFTd6::deltaGzd62 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).

Returns
\((\delta \Gamma_Z/\Gamma_Z)^2\)

Definition at line 2593 of file NPSMEFTd6.cpp.

2594 {
2595  double dWZ = 0.0;
2596 
2597  return (dWZ*dWZ);
2598 }

◆ deltaKgammaNP()

double NPSMEFTd6::deltaKgammaNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).

Returns
\(\delta \kappa_{\gamma}\)

Reimplemented from NPbase.

Definition at line 12207 of file NPSMEFTd6.cpp.

12208 {
12209  double NPdirect;
12210 
12211  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
12212  NPdirect = sqrt( 4.0 * M_PI * aleMz ) / 4.0 / sW2_tree;
12213 
12214  NPdirect = NPdirect * ( (4.0 * sW_tree * cW_tree / sqrt( 4.0 * M_PI * aleMz ) ) * CHWB
12215  - sW_tree * CDHW
12216  - cW_tree * CDHB ) * v2_over_LambdaNP2;
12217 
12218  return NPdirect + dKappaga ;
12219 }
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double dKappaga
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3797
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
complex sqrt(const complex &z)

◆ deltamb()

double NPSMEFTd6::deltamb ( ) const
virtual

The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_b/m_b\)

Definition at line 2421 of file NPSMEFTd6.cpp.

2422 {
2423  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2424  return ( ((quarks[BOTTOM].getMass()) - 4.18) / 4.18 );
2425 }
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222

◆ deltamb2()

double NPSMEFTd6::deltamb2 ( ) const
virtual

The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_b/m_b)^2\)

Definition at line 2427 of file NPSMEFTd6.cpp.

2428 {
2429  return ( 0.0 );
2430 }

◆ deltamc()

double NPSMEFTd6::deltamc ( ) const
virtual

The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_c/m_c\)

Definition at line 2432 of file NPSMEFTd6.cpp.

2433 {
2434  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2435  return ( ((quarks[CHARM].getMass()) - 1.275) / 1.275 );
2436 }
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222

◆ deltamc2()

double NPSMEFTd6::deltamc2 ( ) const
virtual

The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_c/m_c)^2\)

Definition at line 2438 of file NPSMEFTd6.cpp.

2439 {
2440  return ( 0.0 );
2441 }

◆ deltaMh()

double NPSMEFTd6::deltaMh ( ) const
virtual

The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_H/M_H\)

Definition at line 2399 of file NPSMEFTd6.cpp.

2400 {
2401  // Ref. value from SM EW fit 2018
2402  return ( (mHl - 125.1) / 125.1 );
2403 }
double mHl
The Higgs mass in GeV.

◆ deltaMh2()

double NPSMEFTd6::deltaMh2 ( ) const
virtual

The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_H/M_H)^2\)

Definition at line 2405 of file NPSMEFTd6.cpp.

2406 {
2407  return ( 0.0 );
2408 }

◆ deltamt()

double NPSMEFTd6::deltamt ( ) const
virtual

The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_t/m_t\)

Definition at line 2410 of file NPSMEFTd6.cpp.

2411 {
2412  // Ref. value from SM EW fit 2018
2413  return ( (mtpole - 173.2) / 173.2 );
2414 }
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214

◆ deltamt2()

double NPSMEFTd6::deltamt2 ( ) const
virtual

The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_t/m_t)^2\)

Definition at line 2416 of file NPSMEFTd6.cpp.

2417 {
2418  return ( 0.0 );
2419 }

◆ deltamtau()

double NPSMEFTd6::deltamtau ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_\tau/m_\tau\)

Definition at line 2443 of file NPSMEFTd6.cpp.

2444 {
2445  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2446  return ( ((leptons[TAU].getMass()) - 1.77686) / 1.77686 );
2447 }
Definition: QCD.h:607
Particle leptons[6]
An array of Particle objects for the leptons.

◆ deltamtau2()

double NPSMEFTd6::deltamtau2 ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_\tau/m_\tau)^2\)

Definition at line 2449 of file NPSMEFTd6.cpp.

2450 {
2451  return ( 0.0 );
2452 }

◆ deltaMwd6()

double NPSMEFTd6::deltaMwd6 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).

Returns
\(\delta M_W/M_W\)

Definition at line 2509 of file NPSMEFTd6.cpp.

2510 {
2511  return (- 1.0 / 4.0 / (cW2_tree - sW2_tree)
2512  *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
2514  + 2.0 * sW2_tree * DeltaGF()));
2515 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440

◆ deltaMwd62()

double NPSMEFTd6::deltaMwd62 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).

Returns
\((\delta M_W/M_W)^2\)

Definition at line 2517 of file NPSMEFTd6.cpp.

2518 {
2519  double dMW = 0.0;
2520 
2521  return (dMW*dMW);
2522 }

◆ deltaMz()

double NPSMEFTd6::deltaMz ( ) const
virtual

The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_Z/M_Z\)

Definition at line 2388 of file NPSMEFTd6.cpp.

2389 {
2390  // Ref. value from SM EW fit 2018
2391  return ( (Mz - 91.1882) / 91.1882 );
2392 }
double Mz
The mass of the boson in GeV.

◆ deltaMz2()

double NPSMEFTd6::deltaMz2 ( ) const
virtual

The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_Z/M_Z)^2\)

Definition at line 2394 of file NPSMEFTd6.cpp.

2395 {
2396  return ( 0.0 );
2397 }

◆ deltayb_HB()

double NPSMEFTd6::deltayb_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_b\)

Reimplemented from NPbase.

Definition at line 12780 of file NPSMEFTd6.cpp.

12781 {
12782  double mf= (quarks[BOTTOM].getMass());
12783  double ciHB;
12784 
12785  ciHB = - (v()/mf/sqrt(2.0))*CdH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
12786 
12787  return ciHB;
12788 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
complex sqrt(const complex &z)

◆ deltayc_HB()

double NPSMEFTd6::deltayc_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_c\)

Reimplemented from NPbase.

Definition at line 12802 of file NPSMEFTd6.cpp.

12803 {
12804  double mf= (quarks[CHARM].getMass());
12805  double ciHB;
12806 
12807  ciHB = - (v()/mf/sqrt(2.0))*CuH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
12808 
12809  return ciHB;
12810 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
complex sqrt(const complex &z)

◆ deltaymu_HB()

double NPSMEFTd6::deltaymu_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\mu\)

Reimplemented from NPbase.

Definition at line 12813 of file NPSMEFTd6.cpp.

12814 {
12815  double mf= (leptons[MU].getMass());
12816  double ciHB;
12817 
12818  ciHB = - (v()/mf/sqrt(2.0))*CeH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
12819 
12820  return ciHB;
12821 }
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
Particle leptons[6]
An array of Particle objects for the leptons.
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Definition: QCD.h:605
complex sqrt(const complex &z)

◆ deltayt_HB()

double NPSMEFTd6::deltayt_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_t\)

Reimplemented from NPbase.

Definition at line 12769 of file NPSMEFTd6.cpp.

12770 {
12771  double mf= mtpole;
12772  double ciHB;
12773 
12774  ciHB = - (v()/mf/sqrt(2.0))*CuH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
12775 
12776  return ciHB;
12777 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
complex sqrt(const complex &z)

◆ deltaytau_HB()

double NPSMEFTd6::deltaytau_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\tau\)

Reimplemented from NPbase.

Definition at line 12791 of file NPSMEFTd6.cpp.

12792 {
12793  double mf= (leptons[TAU].getMass());
12794  double ciHB;
12795 
12796  ciHB = - (v()/mf/sqrt(2.0))*CeH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
12797 
12798  return ciHB;
12799 }
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
Definition: QCD.h:607
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
Particle leptons[6]
An array of Particle objects for the leptons.
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
complex sqrt(const complex &z)

◆ dxseeWWdcos()

double NPSMEFTd6::dxseeWWdcos ( const double  sqrt_s,
const double  cos 
) const
virtual

The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.

Returns
\(d\sigma/d\cos{\theta}\)

Reimplemented from NPbase.

Definition at line 12233 of file NPSMEFTd6.cpp.

12234 {
12235  double sqrt_sGeV = 1000. * sqrt_s;
12236  double s = sqrt_sGeV * sqrt_sGeV;
12237  double cos2 = cos * cos;
12238  double sin2 = 1.0 - cos2;
12239  double sin = sqrt(sin2);
12240 
12241  double topb = 0.3894*1000000000.0;
12242 
12243 // NC and CC couplings
12244  double gLe, gRe;
12245  gslpp::complex Uenu;
12246 
12247  gLe = -0.5 + sW2_tree + deltaGL_f(leptons[ELECTRON]);
12248  gRe = sW2_tree + deltaGR_f(leptons[ELECTRON]);
12249 
12251  Uenu = 1.0 + Uenu;
12252 
12253 // W mass
12254  double mw;
12255 
12256  mw = Mw();
12257 
12258 // Wigner functions
12259  double d1pp[2],d1mm[2],d1p0[2],d1m0[2],d10p[2],d10m[2],d100[2];
12260 
12261  d1pp[0]=sqrt((1.0 - cos2)/2.0);
12262  d1pp[1]=-sqrt((1.0 - cos2)/2.0);
12263 
12264  d1mm[0]=d1pp[0];
12265  d1mm[1]=d1pp[1];
12266 
12267  d1p0[0]=(1.0 - cos)/2.0;
12268  d1p0[1]=(1.0 + cos)/2.0;
12269 
12270  d1m0[0]=d1p0[1];
12271  d1m0[1]=d1p0[0];
12272 
12273  d10p[0]=d1p0[1];
12274  d10p[1]=d1p0[0];
12275 
12276  d10m[0]=d1p0[0];
12277  d10m[1]=d1p0[1];
12278 
12279  d100[0]=d1pp[0];
12280  d100[1]=d1pp[1];
12281 
12282  gslpp::matrix<double> d1LH(3, 3, 0.0);
12283 
12284  gslpp::matrix<double> d1RH(3, 3, 0.0);
12285 
12286  d1LH.assign(0,0, d1pp[0]);
12287  d1LH.assign(0,1, d1p0[0]);
12288  d1LH.assign(0,2, 0.0);
12289 
12290  d1LH.assign(1,0, d10p[0]);
12291  d1LH.assign(1,1, d100[0]);
12292  d1LH.assign(1,2, d10m[0]);
12293 
12294  d1LH.assign(2,0, 0.0);
12295  d1LH.assign(2,1, d1m0[0]);
12296  d1LH.assign(2,2, d1mm[0]);
12297 
12298  d1RH.assign(0,0, d1pp[1]);
12299  d1RH.assign(0,1, d1p0[1]);
12300  d1RH.assign(0,2, 0.0);
12301 
12302  d1RH.assign(1,0, d10p[1]);
12303  d1RH.assign(1,1, d100[1]);
12304  d1RH.assign(1,2, d10m[1]);
12305 
12306  d1RH.assign(2,0, 0.0);
12307  d1RH.assign(2,1, d1m0[1]);
12308  d1RH.assign(2,2, d1mm[1]);
12309 
12310 // TGC parameterization
12311  double g1Z,g1ga,kZ,kga,lambZ,lambga,g4Z,g4ga,g5Z,g5ga,ktZ,ktga,lambtZ,lambtga;
12312 
12313 // TGC present in the SM
12314  g1Z=1.0 + deltag1ZNP();
12315  g1ga=1.0;
12316  kZ=1.0 + deltag1ZNP() - (sW2_tree/cW2_tree) * deltaKgammaNP();
12317  kga=1.0 + deltaKgammaNP();
12318 // TGC not present in the SM
12319  lambZ=lambdaZNP(); //Check normalization
12320  lambga=lambZ;
12321  g4Z=0.0;
12322  g4ga=0.0;
12323  g5Z=0.0;
12324  g5ga=0.0;
12325  ktZ=0.0;
12326  ktga=0.0;
12327  lambtZ=0.0;
12328  lambtga=0.0;
12329 
12330  double f3Z, f3ga;
12331 
12332  f3Z = g1Z + kZ + lambZ;
12333  f3ga = g1ga + kga + lambga;
12334 
12335  // Kinematic factors
12336  double beta, gamma, gamma2;
12337 
12338  beta = sqrt(1.0 - 4.0 * mw * mw / s);
12339  gamma = sqrt_sGeV/(2.0 * mw);
12340  gamma2= gamma*gamma;
12341 
12342 // J=1 Subamplitudes: Z
12343  gslpp::complex AZpp, AZmm, AZp0, AZm0, AZ0p, AZ0m, AZ00;
12344 
12345  AZpp = gslpp::complex(g1Z + 2.0* gamma2* lambZ, (ktZ + lambtZ - 2.0*lambtZ)/beta , false);
12346  AZmm = gslpp::complex(g1Z + 2.0* gamma2* lambZ, -(ktZ + lambtZ - 2.0*lambtZ)/beta , false);
12347  AZp0 = gslpp::complex(f3Z + beta * g5Z , -g4Z + (ktZ-lambtZ)/beta , false);
12348  AZp0 = gamma * AZp0;
12349  AZm0 = gslpp::complex(f3Z - beta * g5Z , -g4Z - (ktZ-lambtZ)/beta , false);
12350  AZm0 = gamma * AZm0;
12351  AZ0p = gslpp::complex(f3Z - beta * g5Z , g4Z + (ktZ-lambtZ)/beta , false);
12352  AZ0p = gamma * AZ0p;
12353  AZ0m = gslpp::complex(f3Z + beta * g5Z , g4Z - (ktZ-lambtZ)/beta , false);
12354  AZ0m = gamma * AZ0m;
12355  AZ00 = gslpp::complex( g1Z + 2.0*gamma2*kZ, 0.0 , false);
12356 
12357 // Collect in matrices and separate LH and RH
12358  gslpp::matrix<gslpp::complex> AmpZLH(3, 3, 0.0);
12359  gslpp::matrix<gslpp::complex> AmpZRH(3, 3, 0.0);
12360 
12361  AmpZLH.assign(0,0, AZpp * d1LH(0,0) );
12362  AmpZLH.assign(0,1, AZp0 * d1LH(0,1));
12363  AmpZLH.assign(0,2, 0.0);
12364 
12365  AmpZLH.assign(1,0, AZ0p * d1LH(1,0));
12366  AmpZLH.assign(1,1, AZ00 * d1LH(1,1));
12367  AmpZLH.assign(1,2, AZ0m * d1LH(1,2));
12368 
12369  AmpZLH.assign(2,0, 0.0);
12370  AmpZLH.assign(2,1, AZm0 * d1LH(2,1));
12371  AmpZLH.assign(2,2, AZmm * d1LH(2,2));
12372 
12373  AmpZLH = AmpZLH * beta * s/(s-Mz*Mz);
12374 
12375 // Add the correct Zff coupling
12376  AmpZLH = AmpZLH * gLe / sW2_tree;
12377 
12378  AmpZRH.assign(0,0, AZpp * d1RH(0,0) );
12379  AmpZRH.assign(0,1, AZp0 * d1RH(0,1));
12380  AmpZRH.assign(0,2, 0.0);
12381 
12382  AmpZRH.assign(1,0, AZ0p * d1RH(1,0));
12383  AmpZRH.assign(1,1, AZ00 * d1RH(1,1));
12384  AmpZRH.assign(1,2, AZ0m * d1RH(1,2));
12385 
12386  AmpZRH.assign(2,0, 0.0);
12387  AmpZRH.assign(2,1, AZm0 * d1RH(2,1));
12388  AmpZRH.assign(2,2, AZmm * d1RH(2,2));
12389 
12390  AmpZRH = AmpZRH * beta * s/(s-Mz*Mz);
12391 
12392 // Add the correct Zff coupling
12393  AmpZRH = AmpZRH * gRe / sW2_tree;
12394 
12395 // J=1 Subamplitudes: gamma
12396  gslpp::complex Agapp, Agamm, Agap0, Agam0, Aga0p, Aga0m, Aga00;
12397 
12398  Agapp = gslpp::complex(g1ga + 2.0* gamma2* lambga, (ktga + lambtga - 2.0*lambtga)/beta , false);
12399  Agamm = gslpp::complex(g1ga + 2.0* gamma2* lambga, -(ktga + lambtga - 2.0*lambtga)/beta , false);
12400  Agap0 = gslpp::complex(f3ga + beta * g5ga , -g4ga + (ktga-lambtga)/beta , false);
12401  Agap0 = gamma * Agap0;
12402  Agam0 = gslpp::complex(f3ga - beta * g5ga , -g4ga - (ktga-lambtga)/beta , false);
12403  Agam0 = gamma * Agam0;
12404  Aga0p = gslpp::complex(f3ga - beta * g5ga , g4ga + (ktga-lambtga)/beta , false);
12405  Aga0p = gamma * Aga0p;
12406  Aga0m = gslpp::complex(f3ga + beta * g5ga , g4ga - (ktga-lambtga)/beta , false);
12407  Aga0m = gamma * Aga0m;
12408  Aga00 = gslpp::complex( g1ga + 2.0*gamma2*kga, 0.0 , false);
12409 
12410 // Collect in matrices. Here LH = RH, except for the Wigner functions
12411  gslpp::matrix<gslpp::complex> AmpgaLH(3, 3, 0.0);
12412  gslpp::matrix<gslpp::complex> AmpgaRH(3, 3, 0.0);
12413 
12414  AmpgaLH.assign(0,0, Agapp * d1LH(0,0));
12415  AmpgaLH.assign(0,1, Agap0 * d1LH(0,1));
12416  AmpgaLH.assign(0,2, 0.0);
12417 
12418  AmpgaLH.assign(1,0, Aga0p * d1LH(1,0));
12419  AmpgaLH.assign(1,1, Aga00 * d1LH(1,1));
12420  AmpgaLH.assign(1,2, Aga0m * d1LH(1,2));
12421 
12422  AmpgaLH.assign(2,0, 0.0);
12423  AmpgaLH.assign(2,1, Agam0 * d1LH(2,1));
12424  AmpgaLH.assign(2,2, Agamm * d1LH(2,2));
12425 
12426  AmpgaRH.assign(0,0, Agapp * d1RH(0,0));
12427  AmpgaRH.assign(0,1, Agap0 * d1RH(0,1));
12428  AmpgaRH.assign(0,2, 0.0);
12429 
12430  AmpgaRH.assign(1,0, Aga0p * d1RH(1,0));
12431  AmpgaRH.assign(1,1, Aga00 * d1RH(1,1));
12432  AmpgaRH.assign(1,2, Aga0m * d1RH(1,2));
12433 
12434  AmpgaRH.assign(2,0, 0.0);
12435  AmpgaRH.assign(2,1, Agam0 * d1RH(2,1));
12436  AmpgaRH.assign(2,2, Agamm * d1RH(2,2));
12437 
12438  AmpgaLH = -beta * AmpgaLH;
12439  AmpgaRH = -beta * AmpgaRH;
12440 
12441 // J=1 Subamplitudes: neutrino
12442  gslpp::complex Bpp, Bmm, Bp0, Bm0, B0p, B0m, B00;
12443  gslpp::complex Cpp, Cmm, Cp0, Cm0, C0p, C0m, C00;
12444 
12445  Bpp = gslpp::complex(1.0 , 0.0 , false);
12446  Bmm = Bpp;
12447  Bp0 = gslpp::complex( 2.0 * gamma, 0.0 , false);
12448  Bm0 = Bp0;
12449  B0p = Bp0;
12450  B0m = Bp0;
12451  B00 = gslpp::complex( 2.0 * gamma2, 0.0 , false);
12452 
12453  Cpp = gslpp::complex(1.0/gamma2 , 0.0 , false);
12454  Cmm = Cpp;
12455  Cp0 = gslpp::complex( 2.0 * (1.0 + beta)/gamma, 0.0 , false);
12456  Cm0 = gslpp::complex( 2.0 * (1.0 - beta)/gamma, 0.0 , false);
12457  C0p = Cm0;
12458  C0m = Cp0;
12459  C00 = gslpp::complex( 2.0 / gamma2, 0.0 , false);
12460 
12461 // Collect in matrices. Here LH = RH
12462  gslpp::matrix<gslpp::complex> Bnu(3, 3, 0.0);
12463  gslpp::matrix<gslpp::complex> Cnu(3, 3, 0.0);
12464 
12465  Bnu.assign(0,0, Bpp * d1LH(0,0));
12466  Bnu.assign(0,1, Bp0 * d1LH(0,1));
12467  Bnu.assign(0,2, 0.0);
12468 
12469  Bnu.assign(1,0, B0p * d1LH(1,0));
12470  Bnu.assign(1,1, B00 * d1LH(1,1));
12471  Bnu.assign(1,2, B0m * d1LH(1,2));
12472 
12473  Bnu.assign(2,0, 0.0);
12474  Bnu.assign(2,1, Bm0 * d1LH(2,1));
12475  Bnu.assign(2,2, Bmm * d1LH(2,2));
12476 
12477  Cnu.assign(0,0, Cpp * d1LH(0,0));
12478  Cnu.assign(0,1, Cp0 * d1LH(0,1));
12479  Cnu.assign(0,2, 0.0);
12480 
12481  Cnu.assign(1,0, C0p * d1LH(1,0));
12482  Cnu.assign(1,1, C00 * d1LH(1,1));
12483  Cnu.assign(1,2, C0m * d1LH(1,2));
12484 
12485  Cnu.assign(2,0, 0.0);
12486  Cnu.assign(2,1, Cm0 * d1LH(2,1));
12487  Cnu.assign(2,2, Cmm * d1LH(2,2));
12488 
12489 // The matrix with the total J=1 neutrino amplitude (only LH neutrinos)
12490  gslpp::matrix<gslpp::complex> Ampnu1(3, 3, 0.0);
12491 
12492  Ampnu1 = Bnu - Cnu/(1.0 + beta*beta - 2.0 * beta * cos);
12493 
12494  Ampnu1 = Uenu * Uenu.conjugate() * Ampnu1 / (2.0 * beta * sW2_tree);
12495 
12496  gslpp::matrix<gslpp::complex> Ampnu2(3, 3, 0.0);
12497 
12498  Ampnu2.assign(0,2, (1.0 - cos)/2.0 );
12499  Ampnu2.assign(1,1, 0.0);
12500  Ampnu2.assign(2,0, -(1.0 + cos)/2.0);
12501 
12502  Ampnu2 = (8.0 * M_PI * aleMz / sW2_tree)* Uenu * Uenu.conjugate() * Ampnu2 * sin / (1.0 + beta*beta - 2.0*beta*cos);
12503 
12504 // Total amplitudes
12505  gslpp::matrix<gslpp::complex> MRH(3, 3, 0.0);
12506  gslpp::matrix<gslpp::complex> MLH(3, 3, 0.0);
12507 
12508  MRH = sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZRH + AmpgaRH);
12509  MLH = - sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZLH + AmpgaLH + Ampnu1) + Ampnu2;
12510 
12511 // Total amplitude squared and differential cross section (in pb)
12512  gslpp::matrix<double> M2(3, 3, 0.0);
12513  double dxsdcos;
12514 
12515  dxsdcos = 0.0;
12516 
12517  for (int i=0; i<3; i++) {
12518  for (int j=0; j<3; j++) {
12519  M2.assign(i,j, (MRH(i,j)* (MRH(i,j).conjugate())
12520  + MLH(i,j)* (MLH(i,j).conjugate())).real() );
12521 
12522  dxsdcos = dxsdcos + M2(i,j);
12523  }
12524  }
12525 
12526 // Differential cross section in pb
12527  dxsdcos = (topb * beta / 32.0 / M_PI / s) * dxsdcos;
12528 
12529  return dxsdcos;
12530 }
complex cos(const complex &z)
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPSMEFTd6.cpp:2610
virtual double lambdaZNP() const
The new physics contribution to the anomalous triple gauge coupling .
A class for constructing and defining operations on real matrices.
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPSMEFTd6.cpp:2641
complex conjugate() const
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3798
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double Mz
The mass of the boson in GeV.
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPSMEFTd6.cpp:2625
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double gamma
used as an input for FlagWolfenstein = FALSE
virtual double Mw() const
The mass of the boson, .
Definition: NPSMEFTd6.cpp:2501
virtual double deltag1ZNP() const
The new physics contribution to the anomalous triple gauge coupling .
Particle leptons[6]
An array of Particle objects for the leptons.
virtual double deltaKgammaNP() const
The new physics contribution to the anomalous triple gauge coupling .
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
complex sin(const complex &z)
complex sqrt(const complex &z)

◆ dxseeWWdcosBin()

double NPSMEFTd6::dxseeWWdcosBin ( const double  sqrt_s,
const double  cos1,
const double  cos2 
) const
virtual

The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.

Returns
\(\int_{\cos{\theta_1}}^{\cos{\theta_2}} d\sigma/d\cos{\theta}\)

< Gsl integral variable

< Gsl integral variable
< Gsl integral variable

Reimplemented from NPbase.

Definition at line 12532 of file NPSMEFTd6.cpp.

12533 {
12534  double xsWWbin;
12535  double errWW;
12537  gsl_function FR;
12539  FR = convertToGslFunction(boost::bind(&NPSMEFTd6::dxseeWWdcos,&(*this), sqrt_s, _1));
12540 
12541  gsl_integration_cquad(&FR, cos1, cos2, 1.e-5, 1.e-4, w_WW, &xsWWbin, &errWW, NULL);
12542 
12543 // Simple integration for testing
12544 // double cosx;
12545 
12546 // xsWWbin = 0.0;
12547 
12548 // for (int i=1; i<100; i++){
12549 // cosx = cos1 + i*(cos2-cos1)/100;
12550 // xsWWbin = xsWWbin + dxseeWWdcos(sqrt_s, cosx);
12551 // }
12552 
12553 // xsWWbin = xsWWbin + 0.5 * (dxseeWWdcos(sqrt_s, cos1) + dxseeWWdcos(sqrt_s, cos2));
12554 
12555 // xsWWbin = xsWWbin * (cos2-cos1)/100;
12556 
12557 // Compute the BR into e nu, mu nu for one W and into jets for the other
12558  double BRlv, BRjj;
12559 
12560  BRlv = GammaW(leptons[NEUTRINO_1], leptons[ELECTRON]) +
12563 
12564  BRjj = GammaW() - BRlv;
12565 
12566  BRlv = BRlv - GammaW(leptons[NEUTRINO_3], leptons[TAU]);
12567 
12568  BRlv =BRlv / GammaW();
12569 
12570  BRjj =BRjj / GammaW();
12571 
12572 
12573 
12574  return xsWWbin * BRlv * BRjj;
12575 }
gsl_integration_cquad_workspace * w_WW
Definition: NPSMEFTd6.h:3924
virtual double dxseeWWdcos(const double sqrt_s, const double cos) const
The differential distribution for , with , as a function of the polar angle.
Definition: QCD.h:607
virtual double GammaW() const
The total width of the boson, .
Definition: NPSMEFTd6.cpp:2571
gsl_function convertToGslFunction(const F &f)
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: QCD.h:605

◆ f_triangle()

gslpp::complex NPSMEFTd6::f_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

Parameters
[in]

Definition at line 2985 of file NPSMEFTd6.cpp.

2986 {
2987  gslpp::complex tmp;
2988  if (tau >= 1.0) {
2989  tmp = asin(1.0 / sqrt(tau));
2990  return (tmp * tmp);
2991  } else {
2992  tmp = log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i();
2993  return (-0.25 * tmp * tmp);
2994  }
2995 }
static const complex & i()
complex log(const complex &z)
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
complex sqrt(const complex &z)

◆ g_triangle()

gslpp::complex NPSMEFTd6::g_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 2997 of file NPSMEFTd6.cpp.

2998 {
2999  gslpp::complex tmp;
3000  if (tau >= 1.0) {
3001  tmp = sqrt(tau -1.0) * asin(1.0 / sqrt(tau));
3002  return tmp;
3003  } else {
3004  tmp = sqrt(1.0 - tau) * ( log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i() );
3005  return 0.5 * tmp;
3006  }
3007 }
static const complex & i()
complex log(const complex &z)
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
complex sqrt(const complex &z)

◆ GammaHbbRatio()

double NPSMEFTd6::GammaHbbRatio ( ) const

The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 11665 of file NPSMEFTd6.cpp.

11666 {
11667  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11668  double width = 1.0;
11669 
11670  width += deltaGammaHbbRatio1();
11671 
11672  if (FlagQuadraticTerms) {
11673  //Add contributions that are quadratic in the effective coefficients
11674  width += deltaGammaHbbRatio2();
11675  }
11676 
11677  return width;
11678 }
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ GammaHccRatio()

double NPSMEFTd6::GammaHccRatio ( ) const

The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 11599 of file NPSMEFTd6.cpp.

11600 {
11601  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11602  double width = 1.0;
11603 
11604  width += deltaGammaHccRatio1();
11605 
11606  if (FlagQuadraticTerms) {
11607  //Add contributions that are quadratic in the effective coefficients
11608  width += deltaGammaHccRatio2();
11609  }
11610 
11611  return width;
11612 
11613 }
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHgagaRatio()

double NPSMEFTd6::GammaHgagaRatio ( ) const

The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 11418 of file NPSMEFTd6.cpp.

11419 {
11420  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11421  double width = 1.0;
11422 
11423  width += deltaGammaHgagaRatio1();
11424 
11425  if (FlagQuadraticTerms) {
11426  //Add contributions that are quadratic in the effective coefficients
11427  width += deltaGammaHgagaRatio2();
11428  }
11429 
11430  return width;
11431 
11432 }
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ GammaHggRatio()

double NPSMEFTd6::GammaHggRatio ( ) const

The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 9989 of file NPSMEFTd6.cpp.

9990 {
9991  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
9992  double width = 1.0;
9993 
9994  width += deltaGammaHggRatio1();
9995 
9996  if (FlagQuadraticTerms) {
9997  //Add contributions that are quadratic in the effective coefficients
9998  width += deltaGammaHggRatio2();
9999  }
10000 
10001  return width;
10002 
10003 }
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ GammaHmumuRatio()

double NPSMEFTd6::GammaHmumuRatio ( ) const

The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 11494 of file NPSMEFTd6.cpp.

11495 {
11496  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11497  double width = 1.0;
11498 
11499  width += deltaGammaHmumuRatio1();
11500 
11501  if (FlagQuadraticTerms) {
11502  //Add contributions that are quadratic in the effective coefficients
11503  width += deltaGammaHmumuRatio2();
11504  }
11505 
11506  return width;
11507 
11508 }
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHtautauRatio()

double NPSMEFTd6::GammaHtautauRatio ( ) const

The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 11546 of file NPSMEFTd6.cpp.

11547 {
11548  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11549  double width = 1.0;
11550 
11551  width += deltaGammaHtautauRatio1();
11552 
11553  if (FlagQuadraticTerms) {
11554  //Add contributions that are quadratic in the effective coefficients
11555  width += deltaGammaHtautauRatio2();
11556  }
11557 
11558  return width;
11559 
11560 }
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHWffRatio()

double NPSMEFTd6::GammaHWffRatio ( ) const

The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 10331 of file NPSMEFTd6.cpp.

10332 {
10333  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10334  double width = 1.0;
10335 
10336  width += deltaGammaHWffRatio1();
10337 
10338  if (FlagQuadraticTerms) {
10339  //Add contributions that are quadratic in the effective coefficients
10340  width += deltaGammaHWffRatio2();
10341  }
10342 
10343  return width;
10344 
10345 }
double deltaGammaHWffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ GammaHWjjRatio()

double NPSMEFTd6::GammaHWjjRatio ( ) const

The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 10215 of file NPSMEFTd6.cpp.

10216 {
10217  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10218  double width = 1.0;
10219 
10220  width += deltaGammaHWjjRatio1();
10221 
10222  if (FlagQuadraticTerms) {
10223  //Add contributions that are quadratic in the effective coefficients
10224  width += deltaGammaHWjjRatio2();
10225  }
10226 
10227  return width;
10228 
10229 }
double deltaGammaHWjjRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWjjRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ GammaHWlvRatio()

double NPSMEFTd6::GammaHWlvRatio ( ) const

The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 10098 of file NPSMEFTd6.cpp.

10099 {
10100  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10101  double width = 1.0;
10102 
10103  width += deltaGammaHWlvRatio1();
10104 
10105  if (FlagQuadraticTerms) {
10106  //Add contributions that are quadratic in the effective coefficients
10107  width += deltaGammaHWlvRatio2();
10108  }
10109 
10110  return width;
10111 
10112 }
double deltaGammaHWlvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHWlvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...

◆ GammaHWW2l2vRatio()

double NPSMEFTd6::GammaHWW2l2vRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 10154 of file NPSMEFTd6.cpp.

10155 {
10156  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10157  double width = 1.0;
10158 
10159  width += deltaGammaHWW2l2vRatio1();
10160 
10161  if (FlagQuadraticTerms) {
10162  //Add contributions that are quadratic in the effective coefficients
10163  width += deltaGammaHWW2l2vRatio2();
10164  }
10165 
10166  return width;
10167 
10168 }
double deltaGammaHWW2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHWW2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHWW4fRatio()

double NPSMEFTd6::GammaHWW4fRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 10388 of file NPSMEFTd6.cpp.

10389 {
10390  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10391  double width = 1.0;
10392 
10393  width += deltaGammaHWW4fRatio1();
10394 
10395  if (FlagQuadraticTerms) {
10396  //Add contributions that are quadratic in the effective coefficients
10397  width += deltaGammaHWW4fRatio2();
10398  }
10399 
10400  return width;
10401 
10402 }
double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHWW4jRatio()

double NPSMEFTd6::GammaHWW4jRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10271 of file NPSMEFTd6.cpp.

10272 {
10273  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10274  double width = 1.0;
10275 
10276  width += deltaGammaHWW4jRatio1();
10277 
10278  if (FlagQuadraticTerms) {
10279  //Add contributions that are quadratic in the effective coefficients
10280  width += deltaGammaHWW4jRatio2();
10281  }
10282 
10283  return width;
10284 
10285 }
double deltaGammaHWW4jRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHWW4jRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHWWRatio()

double NPSMEFTd6::GammaHWWRatio ( ) const

The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 10050 of file NPSMEFTd6.cpp.

10051 {
10052  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10053  double width = 1.0;
10054 
10055  width += deltaGammaHWWRatio1();
10056 
10057  if (FlagQuadraticTerms) {
10058  //Add contributions that are quadratic in the effective coefficients
10059  width += deltaGammaHWWRatio2();
10060  }
10061 
10062  return width;
10063 
10064 }
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZddRatio()

double NPSMEFTd6::GammaHZddRatio ( ) const

The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zd d)\)/ \(\Gamma(H\to Zd d)_{\mathrm{SM}}\)

Definition at line 11125 of file NPSMEFTd6.cpp.

11126 {
11127  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11128  double width = 1.0;
11129 
11130  width += deltaGammaHZddRatio1();
11131 
11132  if (FlagQuadraticTerms) {
11133  //Add contributions that are quadratic in the effective coefficients
11134  width += deltaGammaHZddRatio2();
11135  }
11136 
11137  return width;
11138 
11139 }
double deltaGammaHZddRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHZddRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...

◆ GammaHZeeRatio()

double NPSMEFTd6::GammaHZeeRatio ( ) const

The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 10565 of file NPSMEFTd6.cpp.

10566 {
10567  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10568  double width = 1.0;
10569 
10570  width += deltaGammaHZeeRatio1();
10571 
10572  if (FlagQuadraticTerms) {
10573  //Add contributions that are quadratic in the effective coefficients
10574  width += deltaGammaHZeeRatio2();
10575  }
10576 
10577  return width;
10578 
10579 }
double deltaGammaHZeeRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHZeeRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...

◆ GammaHZffRatio()

double NPSMEFTd6::GammaHZffRatio ( ) const

The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zff)\)/ \(\Gamma(H\to Zff)_{\mathrm{SM}}\)

Definition at line 11184 of file NPSMEFTd6.cpp.

11185 {
11186  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11187  double width = 1.0;
11188 
11189  width += deltaGammaHZffRatio1();
11190 
11191  if (FlagQuadraticTerms) {
11192  //Add contributions that are quadratic in the effective coefficients
11193  width += deltaGammaHZffRatio2();
11194  }
11195 
11196  return width;
11197 
11198 }
double deltaGammaHZffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
double deltaGammaHZffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZgaRatio()

double NPSMEFTd6::GammaHZgaRatio ( ) const

The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 11333 of file NPSMEFTd6.cpp.

11334 {
11335  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11336  double width = 1.0;
11337 
11338  width += deltaGammaHZgaRatio1();
11339 
11340  if (FlagQuadraticTerms) {
11341  //Add contributions that are quadratic in the effective coefficients
11342  width += deltaGammaHZgaRatio2();
11343  }
11344 
11345  return width;
11346 
11347 }
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZllRatio()

double NPSMEFTd6::GammaHZllRatio ( ) const

The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 10506 of file NPSMEFTd6.cpp.

10507 {
10508  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10509  double width = 1.0;
10510 
10511  width += deltaGammaHZllRatio1();
10512 
10513  if (FlagQuadraticTerms) {
10514  //Add contributions that are quadratic in the effective coefficients
10515  width += deltaGammaHZllRatio2();
10516  }
10517 
10518  return width;
10519 
10520 }
double deltaGammaHZllRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHZllRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZmumuRatio()

double NPSMEFTd6::GammaHZmumuRatio ( ) const

The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 10626 of file NPSMEFTd6.cpp.

10627 {
10628  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10629  double width = 1.0;
10630 
10631  width += deltaGammaHZmumuRatio1();
10632 
10633  if (FlagQuadraticTerms) {
10634  //Add contributions that are quadratic in the effective coefficients
10635  width += deltaGammaHZmumuRatio2();
10636  }
10637 
10638  return width;
10639 
10640 }
double deltaGammaHZmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZuuRatio()

double NPSMEFTd6::GammaHZuuRatio ( ) const

The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zu u)\)/ \(\Gamma(H\to Zu u)_{\mathrm{SM}}\)

Definition at line 11066 of file NPSMEFTd6.cpp.

11067 {
11068  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11069  double width = 1.0;
11070 
11071  width += deltaGammaHZuuRatio1();
11072 
11073  if (FlagQuadraticTerms) {
11074  //Add contributions that are quadratic in the effective coefficients
11075  width += deltaGammaHZuuRatio2();
11076  }
11077 
11078  return width;
11079 
11080 }
double deltaGammaHZuuRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHZuuRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZvvRatio()

double NPSMEFTd6::GammaHZvvRatio ( ) const

The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 10945 of file NPSMEFTd6.cpp.

10946 {
10947  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10948  double width = 1.0;
10949 
10950  width += deltaGammaHZvvRatio1();
10951 
10952  if (FlagQuadraticTerms) {
10953  //Add contributions that are quadratic in the effective coefficients
10954  width += deltaGammaHZvvRatio2();
10955  }
10956 
10957  return width;
10958 
10959 }
double deltaGammaHZvvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZvvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZ2e2muRatio()

double NPSMEFTd6::GammaHZZ2e2muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 10820 of file NPSMEFTd6.cpp.

10821 {
10822  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10823  double width = 1.0;
10824 
10825  width += deltaGammaHZZ2e2muRatio1();
10826 
10827  if (FlagQuadraticTerms) {
10828  //Add contributions that are quadratic in the effective coefficients
10829  width += deltaGammaHZZ2e2muRatio2();
10830  }
10831 
10832  return width;
10833 
10834 }
double deltaGammaHZZ2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZ4dRatio()

double NPSMEFTd6::GammaHZZ4dRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2153 of file NPSMEFTd6.h.

2154  {
2155  return 1.0;
2156  };

◆ GammaHZZ4eRatio()

double NPSMEFTd6::GammaHZZ4eRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 10757 of file NPSMEFTd6.cpp.

10758 {
10759  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10760  double width = 1.0;
10761 
10762  width += deltaGammaHZZ4eRatio1();
10763 
10764  if (FlagQuadraticTerms) {
10765  //Add contributions that are quadratic in the effective coefficients
10766  width += deltaGammaHZZ4eRatio2();
10767  }
10768 
10769  return width;
10770 
10771 }
double deltaGammaHZZ4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZ4fRatio()

double NPSMEFTd6::GammaHZZ4fRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 11247 of file NPSMEFTd6.cpp.

11248 {
11249  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11250  double width = 1.0;
11251 
11252  width += deltaGammaHZZ4fRatio1();
11253 
11254  if (FlagQuadraticTerms) {
11255  //Add contributions that are quadratic in the effective coefficients
11256  width += deltaGammaHZZ4fRatio2();
11257  }
11258 
11259  return width;
11260 
11261 }
double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...

◆ GammaHZZ4lRatio()

double NPSMEFTd6::GammaHZZ4lRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 10687 of file NPSMEFTd6.cpp.

10688 {
10689  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10690  double width = 1.0;
10691 
10692  width += deltaGammaHZZ4lRatio1();
10693 
10694  if (FlagQuadraticTerms) {
10695  //Add contributions that are quadratic in the effective coefficients
10696  width += deltaGammaHZZ4lRatio2();
10697  }
10698 
10699  return width;
10700 
10701 }
double deltaGammaHZZ4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
double deltaGammaHZZ4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZ4muRatio()

double NPSMEFTd6::GammaHZZ4muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 10882 of file NPSMEFTd6.cpp.

10883 {
10884  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10885  double width = 1.0;
10886 
10887  width += deltaGammaHZZ4muRatio1();
10888 
10889  if (FlagQuadraticTerms) {
10890  //Add contributions that are quadratic in the effective coefficients
10891  width += deltaGammaHZZ4muRatio2();
10892  }
10893 
10894  return width;
10895 
10896 }
double deltaGammaHZZ4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZ4uRatio()

double NPSMEFTd6::GammaHZZ4uRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4u)\)/ \(\Gamma(H\to ZZ* \to 4u)_{\mathrm{SM}}\)

Definition at line 2138 of file NPSMEFTd6.h.

2139  {
2140  return 1.0;
2141  };

◆ GammaHZZ4vRatio()

double NPSMEFTd6::GammaHZZ4vRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11003 of file NPSMEFTd6.cpp.

11004 {
11005  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11006  double width = 1.0;
11007 
11008  width += deltaGammaHZZ4vRatio1();
11009 
11010  if (FlagQuadraticTerms) {
11011  //Add contributions that are quadratic in the effective coefficients
11012  width += deltaGammaHZZ4vRatio2();
11013  }
11014 
11015  return width;
11016 
11017 }
double deltaGammaHZZ4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZ4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaHZZRatio()

double NPSMEFTd6::GammaHZZRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 10458 of file NPSMEFTd6.cpp.

10459 {
10460  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10461  double width = 1.0;
10462 
10463  width += deltaGammaHZZRatio1();
10464 
10465  if (FlagQuadraticTerms) {
10466  //Add contributions that are quadratic in the effective coefficients
10467  width += deltaGammaHZZRatio2();
10468  }
10469 
10470  return width;
10471 
10472 }
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903

◆ GammaW() [1/2]

double NPSMEFTd6::GammaW ( const Particle  fi,
const Particle  fj 
) const
virtual

A partial decay width of the \(W\) boson decay into a SM fermion pair.

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\Gamma^W_{ij}\)

Reimplemented from NPbase.

Definition at line 2553 of file NPSMEFTd6.cpp.

2554 {
2555  return ( trueSM.GammaW(fi, fj) + deltaGamma_Wff(fi, fj) );
2556 }
virtual double deltaGamma_Wff(const Particle fi, const Particle fj) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPSMEFTd6.cpp:2524
StandardModel trueSM
Definition: NPbase.h:1902
virtual double GammaW(const Particle fi, const Particle fj) const
A partial decay width of the boson decay into a SM fermion pair.

◆ GammaW() [2/2]

double NPSMEFTd6::GammaW ( ) const
virtual

The total width of the \(W\) boson, \(\Gamma_W\).

Returns
\(\Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 2571 of file NPSMEFTd6.cpp.

2572 {
2573  return ( trueSM.GammaW() + deltaGamma_W() );
2574 }
StandardModel trueSM
Definition: NPbase.h:1902
virtual double deltaGamma_W() const
The new physics contribution to the total decay width of the boson, .
Definition: NPSMEFTd6.cpp:2558
virtual double GammaW(const Particle fi, const Particle fj) const
A partial decay width of the boson decay into a SM fermion pair.

◆ getCed_1123()

double NPSMEFTd6::getCed_1123 ( ) const
inline

Return NP coeff Ced_1123.

Returns
\( Ced_1123 \)

Definition at line 912 of file NPSMEFTd6.h.

912  {
913  return Ced_1123;
914  }
double Ced_1123
Definition: NPSMEFTd6.h:3614

◆ getCed_2223()

double NPSMEFTd6::getCed_2223 ( ) const
inline

Return NP coeff Ced_2223.

Returns
\( Ced_2223 \)

Definition at line 920 of file NPSMEFTd6.h.

920  {
921  return Ced_2223;
922  }
double Ced_2223
Definition: NPSMEFTd6.h:3614

◆ getCeu_1133()

double NPSMEFTd6::getCeu_1133 ( ) const
inline

Return NP coeff Ceu_1133.

Returns
\( Ceu_1133 \)

Definition at line 976 of file NPSMEFTd6.h.

976  {
977  return Ceu_1133;
978  }
double Ceu_1133
Definition: NPSMEFTd6.h:3609

◆ getCeu_2233()

double NPSMEFTd6::getCeu_2233 ( ) const
inline

Return NP coeff Ceu_2233.

Returns
\( Ceu_2233 \)

Definition at line 984 of file NPSMEFTd6.h.

984  {
985  return Ceu_2233;
986  }
double Ceu_2233
Definition: NPSMEFTd6.h:3610

◆ getCHe_11()

double NPSMEFTd6::getCHe_11 ( ) const
inline

Return NP coeff CHe_11.

Returns
\( CHe_11 \)

Definition at line 960 of file NPSMEFTd6.h.

960  {
961  return CHe_11;
962  }
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462

◆ getCHe_22()

double NPSMEFTd6::getCHe_22 ( ) const
inline

Return NP coeff CHe_22.

Returns
\( CHe_22 \)

Definition at line 968 of file NPSMEFTd6.h.

968  {
969  return CHe_22;
970  }
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465

◆ getCHL1_11()

double NPSMEFTd6::getCHL1_11 ( ) const
inline

Return NP coeff CHL1_11.

Returns
\( CHL1_11 \)

Definition at line 928 of file NPSMEFTd6.h.

928  {
929  return CHL1_11;
930  }
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444

◆ getCHL1_22()

double NPSMEFTd6::getCHL1_22 ( ) const
inline

Return NP coeff CHL1_22.

Returns
\( CHL1_22 \)

Definition at line 936 of file NPSMEFTd6.h.

936  {
937  return CHL1_22;
938  }
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447

◆ getCHL3_11()

double NPSMEFTd6::getCHL3_11 ( ) const
inline

Return NP coeff CHL3_11.

Returns
\( CHL3_11 \)

Definition at line 944 of file NPSMEFTd6.h.

944  {
945  return CHL3_11;
946  }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453

◆ getCHL3_22()

double NPSMEFTd6::getCHL3_22 ( ) const
inline

Return NP coeff CHL3_22.

Returns
\( CHL3_22 \)

Definition at line 952 of file NPSMEFTd6.h.

952  {
953  return CHL3_22;
954  }
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456

◆ getCLd_1123()

double NPSMEFTd6::getCLd_1123 ( ) const
inline

Return NP coeff CLd_1123.

Returns
\( CLd_1123 \)

Definition at line 896 of file NPSMEFTd6.h.

896  {
897  return CLd_1123;
898  }
double CLd_1123
Definition: NPSMEFTd6.h:3626

◆ getCLd_2223()

double NPSMEFTd6::getCLd_2223 ( ) const
inline

Return NP coeff CLd_2223.

Returns
\( CLd_2223 \)

Definition at line 904 of file NPSMEFTd6.h.

904  {
905  return CLd_2223;
906  }
double CLd_2223
Definition: NPSMEFTd6.h:3626

◆ getCLedQ_11()

double NPSMEFTd6::getCLedQ_11 ( ) const
inline

Return NP coeff CLedq_11.

Returns
\( CLedq_11 \)

Definition at line 1008 of file NPSMEFTd6.h.

1008  {
1009  return CLedQ_11;
1010  }
double CLedQ_11
Definition: NPSMEFTd6.h:3633

◆ getCLedQ_22()

double NPSMEFTd6::getCLedQ_22 ( ) const
inline

Return NP coeff CLedq_22.

Returns
\( CLedq_22 \)

Definition at line 1016 of file NPSMEFTd6.h.

1016  {
1017  return CLedQ_22;
1018  }
double CLedQ_22
Definition: NPSMEFTd6.h:3633

◆ getCLQ1_1123()

double NPSMEFTd6::getCLQ1_1123 ( ) const
inline

Return NP coeff CLQ1_1123.

Returns
\( CLQ1_1123 \)

Definition at line 864 of file NPSMEFTd6.h.

864  {
865  return CLQ1_1123;
866  }
double CLQ1_1123
Definition: NPSMEFTd6.h:3597

◆ getCLQ1_2223()

double NPSMEFTd6::getCLQ1_2223 ( ) const
inline

Return NP coeff CLQ1_2223.

Returns
\( CLQ1_2223 \)

Definition at line 872 of file NPSMEFTd6.h.

872  {
873  return CLQ1_2223;
874  }
double CLQ1_2223
Definition: NPSMEFTd6.h:3597

◆ getCLQ3_1123()

double NPSMEFTd6::getCLQ3_1123 ( ) const
inline

Return NP coeff CLQ3_1123.

Returns
\( CLQ3_1123 \)

Definition at line 880 of file NPSMEFTd6.h.

880  {
881  return CLQ3_1123;
882  }
double CLQ3_1123
Definition: NPSMEFTd6.h:3602

◆ getCLQ3_2223()

double NPSMEFTd6::getCLQ3_2223 ( ) const
inline

Return NP coeff CLQ3_2223.

Returns
\( CLQ3_2223 \)

Definition at line 888 of file NPSMEFTd6.h.

888  {
889  return CLQ3_2223;
890  }
double CLQ3_2223
Definition: NPSMEFTd6.h:3602

◆ getCLu_1133()

double NPSMEFTd6::getCLu_1133 ( ) const
inline

Return NP coeff CLu_1133.

Returns
\( CLu_1133 \)

Definition at line 992 of file NPSMEFTd6.h.

992  {
993  return CLu_1133;
994  }
double CLu_1133
Definition: NPSMEFTd6.h:3621

◆ getCLu_2233()

double NPSMEFTd6::getCLu_2233 ( ) const
inline

Return NP coeff CLu_2233.

Returns
\( CLu_2233 \)

Definition at line 1000 of file NPSMEFTd6.h.

1000  {
1001  return CLu_2233;
1002  }
double CLu_2233
Definition: NPSMEFTd6.h:3622

◆ getCpLedQ_11()

double NPSMEFTd6::getCpLedQ_11 ( ) const
inline

Return NP coeff CpLedq_11.

Returns
\( CpLedq_11 \)

Definition at line 1024 of file NPSMEFTd6.h.

1024  {
1025  return CpLedQ_11;
1026  }
double CpLedQ_11
Definition: NPSMEFTd6.h:3633

◆ getCpLedQ_22()

double NPSMEFTd6::getCpLedQ_22 ( ) const
inline

Return NP coeff CpLedq_22.

Returns
\( CpLedq \)

Definition at line 1032 of file NPSMEFTd6.h.

1032  {
1033  return CpLedQ_22;
1034  }
double CpLedQ_22
Definition: NPSMEFTd6.h:3633

◆ getCQe_2311()

double NPSMEFTd6::getCQe_2311 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2322 \)

Definition at line 848 of file NPSMEFTd6.h.

848  {
849  return CQe_2311;
850  }
double CQe_2311
Definition: NPSMEFTd6.h:3631

◆ getCQe_2322()

double NPSMEFTd6::getCQe_2322 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2311 \)

Definition at line 856 of file NPSMEFTd6.h.

856  {
857  return CQe_2322;
858  }
double CQe_2322
Definition: NPSMEFTd6.h:3631

◆ getLambda_NP()

double NPSMEFTd6::getLambda_NP ( ) const
inline

Return Lambda_NP.

Returns
\( Lambda_NP \)

Definition at line 840 of file NPSMEFTd6.h.

840  {
841  return Lambda_NP;
842  }
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:3634

◆ getMatching()

virtual NPSMEFTd6Matching& NPSMEFTd6::getMatching ( ) const
inlinevirtual

A method to get the Matching object for this model.

Returns
The matching object for this model

Reimplemented from StandardModel.

Definition at line 829 of file NPSMEFTd6.h.

830  {
831  return NPSMEFTd6M.getObj();
832  }
Matching< NPSMEFTd6Matching, NPSMEFTd6 > NPSMEFTd6M
Definition: NPSMEFTd6.h:3427
T & getObj()
Definition: Matching.h:16

◆ I_triangle_1()

gslpp::complex NPSMEFTd6::I_triangle_1 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3009 of file NPSMEFTd6.cpp.

3010 {
3011  gslpp::complex tmp;
3012 
3013  tmp = ( tau*lambda * (f_triangle(tau)- f_triangle(lambda)) + 2.0 * tau * (g_triangle(tau)- g_triangle(lambda)) ) / (tau-lambda);
3014 
3015  tmp = tau*lambda * ( 1.0 + tmp ) / (2.0*(tau-lambda));
3016 
3017  return tmp;
3018 }
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:2985
double lambda
The CKM parameter in the Wolfenstein parameterization.
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
gslpp::complex g_triangle(const double tau) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:2997

◆ I_triangle_2()

gslpp::complex NPSMEFTd6::I_triangle_2 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3020 of file NPSMEFTd6.cpp.

3021 {
3022  gslpp::complex tmp;
3023 
3024  tmp = - 0.5 * tau*lambda * (f_triangle(tau)- f_triangle(lambda)) / (tau-lambda);
3025 
3026  return tmp;
3027 }
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:2985
double lambda
The CKM parameter in the Wolfenstein parameterization.
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35

◆ kappaAeff()

double NPSMEFTd6::kappaAeff ( ) const
virtual

The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).

Returns
\(\kappa_{A,eff}\)

Reimplemented from NPbase.

Definition at line 12755 of file NPSMEFTd6.cpp.

12756 {
12757  return sqrt(GammaHgagaRatio());
12758 }
double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappabeff()

double NPSMEFTd6::kappabeff ( ) const
virtual

The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).

Returns
\(\kappa_{b,eff}\)

Reimplemented from NPbase.

Definition at line 12735 of file NPSMEFTd6.cpp.

12736 {
12737  return sqrt(GammaHbbRatio());
12738 }
double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappaceff()

double NPSMEFTd6::kappaceff ( ) const
virtual

The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).

Returns
\(\kappa_{c,eff}\)

Reimplemented from NPbase.

Definition at line 12730 of file NPSMEFTd6.cpp.

12731 {
12732  return sqrt(GammaHccRatio());
12733 }
double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappaGeff()

double NPSMEFTd6::kappaGeff ( ) const
virtual

The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).

Returns
\(\kappa_{G,eff}\)

Reimplemented from NPbase.

Definition at line 12740 of file NPSMEFTd6.cpp.

12741 {
12742  return sqrt(GammaHggRatio());
12743 }
double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9989
complex sqrt(const complex &z)

◆ kappamueff()

double NPSMEFTd6::kappamueff ( ) const
virtual

The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).

Returns
\(\kappa_{\mu,eff}\)

Reimplemented from NPbase.

Definition at line 12720 of file NPSMEFTd6.cpp.

12721 {
12722  return sqrt(GammaHmumuRatio());
12723 }
double GammaHmumuRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappataueff()

double NPSMEFTd6::kappataueff ( ) const
virtual

The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).

Returns
\(\kappa_{\tau,eff}\)

Reimplemented from NPbase.

Definition at line 12725 of file NPSMEFTd6.cpp.

12726 {
12727  return sqrt(GammaHtautauRatio());
12728 }
double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappaWeff()

double NPSMEFTd6::kappaWeff ( ) const
virtual

The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).

Returns
\(\kappa_{W,eff}\)

Reimplemented from NPbase.

Definition at line 12750 of file NPSMEFTd6.cpp.

12751 {
12752  return sqrt(GammaHWWRatio());
12753 }
double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappaZAeff()

double NPSMEFTd6::kappaZAeff ( ) const
virtual

The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).

Returns
\(\kappa_{ZA,eff}\)

Reimplemented from NPbase.

Definition at line 12760 of file NPSMEFTd6.cpp.

12761 {
12762  return sqrt(GammaHZgaRatio());
12763 }
double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ kappaZeff()

double NPSMEFTd6::kappaZeff ( ) const
virtual

The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).

Returns
\(\kappa_{Z,eff}\)

Reimplemented from NPbase.

Definition at line 12745 of file NPSMEFTd6.cpp.

12746 {
12747  return sqrt(GammaHZZRatio());
12748 }
double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
complex sqrt(const complex &z)

◆ lambdaZNP()

double NPSMEFTd6::lambdaZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).

Returns
\(\lambda_{Z}\)

Reimplemented from NPbase.

Definition at line 12221 of file NPSMEFTd6.cpp.

12222 {
12223  double NPdirect;
12224 
12225  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
12226  NPdirect = - (3.0 / 2.0) * (sqrt( 4.0 * M_PI * aleMz ) / sW_tree) * CW * v2_over_LambdaNP2;
12227 
12228  return NPdirect + lambZ ;
12229 }
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3798
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3430
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
complex sqrt(const complex &z)

◆ lambz_HB()

double NPSMEFTd6::lambz_HB ( ) const
virtual

The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\lambda_{z}\)

Reimplemented from NPbase.

Definition at line 12890 of file NPSMEFTd6.cpp.

12891 {
12892  double ciHB;
12893 
12894  ciHB = -(3.0/2.0)*(eeMz/sW_tree)*CW*v2_over_LambdaNP2;
12895 
12896  return ciHB;
12897 }
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3430
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ mueeHvv()

double NPSMEFTd6::mueeHvv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 3754 of file NPSMEFTd6.cpp.

3755 {
3756  double mu = 1.0;
3757 
3758  double C1 = 0.0;
3759 
3760 // For the Higgs trilinear dependence assume the WBF mechanism dominates
3761 
3762  if (sqrt_s == 0.240) {
3763 
3764  C1 = 0.0064;
3765 
3766  mu +=
3767  +121539. * CHbox / LambdaNP2
3768  +328845. * CHL1_11 / LambdaNP2
3769  -37798.9 * CHe_11 / LambdaNP2
3770  +279733. * CHL3_11 / LambdaNP2
3771  -196039. * CHD / LambdaNP2
3772  -70718.5 * CHB / LambdaNP2
3773  +29671.9 * CHW / LambdaNP2
3774  -401378. * CHWB / LambdaNP2
3775  -23969.3 * CDHB / LambdaNP2
3776  -1814.47 * CDHW / LambdaNP2
3777  -4.698 * DeltaGF()
3778  -5.463 * deltaMwd6()
3779  ;
3780 
3781  // Add modifications due to small variations of the SM parameters
3782  mu += cHSM * (
3783  +4.842 * deltaMz()
3784  -2.535 * deltaMh()
3785  -0.528 * deltaaMZ()
3786  +3.46 * deltaGmu() );
3787 
3788  if (FlagQuadraticTerms) {
3789  //Add contributions that are quadratic in the effective coefficients
3790  mu += 0.0;
3791  }
3792 
3793  } else if (sqrt_s == 0.250) {
3794 
3795  C1 = 0.0064;
3796 
3797  mu +=
3798  +120627. * CHbox / LambdaNP2
3799  +256825. * CHL1_11 / LambdaNP2
3800  -38677.5 * CHe_11 / LambdaNP2
3801  +175735. * CHL3_11 / LambdaNP2
3802  -201059. * CHD / LambdaNP2
3803  -57405. * CHB / LambdaNP2
3804  -9860.82 * CHW / LambdaNP2
3805  -403474. * CHWB / LambdaNP2
3806  -20447.1 * CDHB / LambdaNP2
3807  -9672.74 * CDHW / LambdaNP2
3808  -4.656 * DeltaGF()
3809  -5.633 * deltaMwd6()
3810  ;
3811 
3812  // Add modifications due to small variations of the SM parameters
3813  mu += cHSM * (
3814  +4.194 * deltaMz()
3815  -2.783 * deltaMh()
3816  -0.477 * deltaaMZ()
3817  +3.414 * deltaGmu() );
3818 
3819  if (FlagQuadraticTerms) {
3820  //Add contributions that are quadratic in the effective coefficients
3821  mu += 0.0;
3822  }
3823 
3824  } else if (sqrt_s == 0.350) {
3825 
3826  C1 = 0.0062;
3827 
3828  mu +=
3829  +120666. * CHbox / LambdaNP2
3830  -19184.6 * CHL1_11 / LambdaNP2
3831  -27432.1 * CHe_11 / LambdaNP2
3832  -238244. * CHL3_11 / LambdaNP2
3833  -204898. * CHD / LambdaNP2
3834  +11833.5 * CHB / LambdaNP2
3835  -94273.3 * CHW / LambdaNP2
3836  -377703. * CHWB / LambdaNP2
3837  +1111.63 * CDHB / LambdaNP2
3838  -31735.2 * CDHW / LambdaNP2
3839  -4.669 * DeltaGF()
3840  -5.329 * deltaMwd6()
3841  ;
3842 
3843  // Add modifications due to small variations of the SM parameters
3844  mu += cHSM * (
3845  +3.738 * deltaMz()
3846  -1.994 * deltaMh()
3847  -0.537 * deltaaMZ()
3848  +3.484 * deltaGmu() );
3849 
3850  if (FlagQuadraticTerms) {
3851  //Add contributions that are quadratic in the effective coefficients
3852  mu += 0.0;
3853  }
3854 
3855  } else if (sqrt_s == 0.365) {
3856 
3857  C1 = 0.0062; // Use the same as 350 GeV
3858 
3859  mu +=
3860  +120864. * CHbox / LambdaNP2
3861  -24430. * CHL1_11 / LambdaNP2
3862  -24398.7 * CHe_11 / LambdaNP2
3863  -253414. * CHL3_11 / LambdaNP2
3864  -204817. * CHD / LambdaNP2
3865  +12826.5 * CHB / LambdaNP2
3866  -93455. * CHW / LambdaNP2
3867  -377489. * CHWB / LambdaNP2
3868  +1693.48 * CDHB / LambdaNP2
3869  -32834.7 * CDHW / LambdaNP2
3870  -4.68 * DeltaGF()
3871  -5.265 * deltaMwd6()
3872  ;
3873 
3874  // Add modifications due to small variations of the SM parameters
3875  mu += cHSM * (
3876  +3.834 * deltaMz()
3877  -1.867 * deltaMh()
3878  -0.556 * deltaaMZ()
3879  +3.512 * deltaGmu() );
3880 
3881  if (FlagQuadraticTerms) {
3882  //Add contributions that are quadratic in the effective coefficients
3883  mu += 0.0;
3884  }
3885 
3886  } else if (sqrt_s == 0.380) {
3887 
3888  C1 = 0.0062; // Use the same as 350 GeV
3889 
3890  mu +=
3891  +120775. * CHbox / LambdaNP2
3892  -27548.7 * CHL1_11 / LambdaNP2
3893  -22022.3 * CHe_11 / LambdaNP2
3894  -266603. * CHL3_11 / LambdaNP2
3895  -204782. * CHD / LambdaNP2
3896  +13052.3 * CHB / LambdaNP2
3897  -92560.2 * CHW / LambdaNP2
3898  -377461. * CHWB / LambdaNP2
3899  +1916.19 * CDHB / LambdaNP2
3900  -33824.9 * CDHW / LambdaNP2
3901  -4.684 * DeltaGF()
3902  -5.221 * deltaMwd6()
3903  ;
3904 
3905  // Add modifications due to small variations of the SM parameters
3906  mu += cHSM * (
3907  +3.931 * deltaMz()
3908  -1.75 * deltaMh()
3909  -0.574 * deltaaMZ()
3910  +3.532 * deltaGmu() );
3911 
3912  if (FlagQuadraticTerms) {
3913  //Add contributions that are quadratic in the effective coefficients
3914  mu += 0.0;
3915  }
3916 
3917  } else if (sqrt_s == 0.500) {
3918 
3919  C1 = 0.0061;
3920 
3921  mu +=
3922  +120683. * CHbox / LambdaNP2
3923  -26906.2 * CHL1_11 / LambdaNP2
3924  -11055.8 * CHe_11 / LambdaNP2
3925  -326940. * CHL3_11 / LambdaNP2
3926  -204335. * CHD / LambdaNP2
3927  +10505.8 * CHB / LambdaNP2
3928  -82453.1 * CHW / LambdaNP2
3929  -378407. * CHWB / LambdaNP2
3930  +1889.64 * CDHB / LambdaNP2
3931  -41332.3 * CDHW / LambdaNP2
3932  -4.705 * DeltaGF()
3933  -4.943 * deltaMwd6()
3934  ;
3935 
3936  // Add modifications due to small variations of the SM parameters
3937  mu += cHSM * (
3938  +4.412 * deltaMz()
3939  -1.191 * deltaMh()
3940  -0.659 * deltaaMZ()
3941  +3.633 * deltaGmu() );
3942 
3943  if (FlagQuadraticTerms) {
3944  //Add contributions that are quadratic in the effective coefficients
3945  mu += 0.0;
3946  }
3947 
3948  } else if (sqrt_s == 1.0) {
3949 
3950  C1 = 0.0059;
3951 
3952  mu +=
3953  +120462. * CHbox / LambdaNP2
3954  -9025.99 * CHL1_11 / LambdaNP2
3955  -3124.38 * CHe_11 / LambdaNP2
3956  -454282. * CHL3_11 / LambdaNP2
3957  -204077. * CHD / LambdaNP2
3958  +3421.94 * CHB / LambdaNP2
3959  -61892.5 * CHW / LambdaNP2
3960  -379786. * CHWB / LambdaNP2
3961  +396.747 * CDHB / LambdaNP2
3962  -63826.6 * CDHW / LambdaNP2
3963  -4.711 * DeltaGF()
3964  -4.587 * deltaMwd6()
3965  ;
3966 
3967  // Add modifications due to small variations of the SM parameters
3968  mu += cHSM * (
3969  +4.969 * deltaMz()
3970  -0.583 * deltaMh()
3971  -0.745 * deltaaMZ()
3972  +3.729 * deltaGmu() );
3973 
3974  if (FlagQuadraticTerms) {
3975  //Add contributions that are quadratic in the effective coefficients
3976  mu += 0.0;
3977  }
3978 
3979  } else if (sqrt_s == 1.4) {
3980 
3981  C1 = 0.0058;
3982 
3983  mu +=
3984  +120512. * CHbox / LambdaNP2
3985  -4746.27 * CHL1_11 / LambdaNP2
3986  -2212.55 * CHe_11 / LambdaNP2
3987  -521829. * CHL3_11 / LambdaNP2
3988  -204054. * CHD / LambdaNP2
3989  +1891.37 * CHB / LambdaNP2
3990  -54492.9 * CHW / LambdaNP2
3991  -379916. * CHWB / LambdaNP2
3992  +142.745 * CDHB / LambdaNP2
3993  -75976. * CDHW / LambdaNP2
3994  -4.712 * DeltaGF()
3995  -4.486 * deltaMwd6()
3996  ;
3997 
3998  // Add modifications due to small variations of the SM parameters
3999  mu += cHSM * (
4000  +5.108 * deltaMz()
4001  -0.447 * deltaMh()
4002  -0.767 * deltaaMZ()
4003  +3.751 * deltaGmu() );
4004 
4005  if (FlagQuadraticTerms) {
4006  //Add contributions that are quadratic in the effective coefficients
4007  mu += 0.0;
4008  }
4009 
4010  } else if (sqrt_s == 1.5) {
4011 
4012  C1 = 0.0058;// Use the same as 1400 GeV
4013 
4014  mu +=
4015  +120512. * CHbox / LambdaNP2
4016  -4105.67 * CHL1_11 / LambdaNP2
4017  -2086.49 * CHe_11 / LambdaNP2
4018  -536150. * CHL3_11 / LambdaNP2
4019  -204072. * CHD / LambdaNP2
4020  +1682.65 * CHB / LambdaNP2
4021  -53138.1 * CHW / LambdaNP2
4022  -379943. * CHWB / LambdaNP2
4023  +134.612 * CDHB / LambdaNP2
4024  -78546.2 * CDHW / LambdaNP2
4025  -4.711 * DeltaGF()
4026  -4.469 * deltaMwd6()
4027  ;
4028 
4029  // Add modifications due to small variations of the SM parameters
4030  mu += cHSM * (
4031  +5.132 * deltaMz()
4032  -0.424 * deltaMh()
4033  -0.773 * deltaaMZ()
4034  +3.757 * deltaGmu() );
4035 
4036  if (FlagQuadraticTerms) {
4037  //Add contributions that are quadratic in the effective coefficients
4038  mu += 0.0;
4039  }
4040 
4041  } else if (sqrt_s == 3.0) {
4042 
4043  C1 = 0.0057;
4044 
4045  mu +=
4046  +120404. * CHbox / LambdaNP2
4047  -1215.14 * CHL1_11 / LambdaNP2
4048  -1382.75 * CHe_11 / LambdaNP2
4049  -686451. * CHL3_11 / LambdaNP2
4050  -204039. * CHD / LambdaNP2
4051  +293.31 * CHB / LambdaNP2
4052  -41440.6 * CHW / LambdaNP2
4053  -380130. * CHWB / LambdaNP2
4054  -272.36 * CDHB / LambdaNP2
4055  -104900. * CDHW / LambdaNP2
4056  -4.706 * DeltaGF()
4057  -4.343 * deltaMwd6()
4058  ;
4059 
4060  // Add modifications due to small variations of the SM parameters
4061  mu += cHSM * (
4062  +5.307 * deltaMz()
4063  -0.283 * deltaMh()
4064  -0.802 * deltaaMZ()
4065  +3.789 * deltaGmu() );
4066 
4067  if (FlagQuadraticTerms) {
4068  //Add contributions that are quadratic in the effective coefficients
4069  mu += 0.0;
4070  }
4071 
4072  } else
4073  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvv()");
4074 
4075  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
4076  mu += eeeWBFint + eeeWBFpar;
4077 
4078 // Linear contribution from Higgs self-coupling
4079  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
4080 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
4082 
4083  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
4084 
4085  return mu;
4086 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeHvvPol()

double NPSMEFTd6::mueeHvvPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 4089 of file NPSMEFTd6.cpp.

4090 {
4091  double mu = 1.0;
4092 
4093  double C1 = 0.0;
4094 
4095 // For the Higgs trilinear dependence assume the WBF mechanism dominates
4096 
4097  if (sqrt_s == 0.240) {
4098 
4099  C1 = 0.0064;
4100 
4101  if (Pol_em == 80. && Pol_ep == -30.){
4102  mu +=
4103  +121180. * CHbox / LambdaNP2
4104  +221479. * CHL1_11 / LambdaNP2
4105  -508958. * CHe_11 / LambdaNP2
4106  +220003. * CHL3_11 / LambdaNP2
4107  -149238. * CHD / LambdaNP2
4108  +24268.3 * CHB / LambdaNP2
4109  -32411.5 * CHW / LambdaNP2
4110  -194663. * CHWB / LambdaNP2
4111  +29267.1 * CDHB / LambdaNP2
4112  -11610.1 * CDHW / LambdaNP2
4113  -3.633 * DeltaGF()
4114  -4.394 * deltaMwd6()
4115  ;
4116 
4117  // Add modifications due to small variations of the SM parameters
4118  mu += cHSM * ( +2.975 * deltaMz()
4119  -2.624 * deltaMh()
4120  +0.379 * deltaaMZ()
4121  +2.282 * deltaGmu() );
4122 
4123  } else if (Pol_em == -80. && Pol_ep == 30.){
4124  mu +=
4125  +121456. * CHbox / LambdaNP2
4126  +337881. * CHL1_11 / LambdaNP2
4127  +931.718 * CHe_11 / LambdaNP2
4128  +283908. * CHL3_11 / LambdaNP2
4129  -199920. * CHD / LambdaNP2
4130  -78796.8 * CHB / LambdaNP2
4131  +34606.7 * CHW / LambdaNP2
4132  -418335. * CHWB / LambdaNP2
4133  -28484. * CDHB / LambdaNP2
4134  -1197.92 * CDHW / LambdaNP2
4135  -4.781 * DeltaGF()
4136  -5.537 * deltaMwd6()
4137  ;
4138 
4139  // Add modifications due to small variations of the SM parameters
4140  mu += cHSM * ( +5.005 * deltaMz()
4141  -2.529 * deltaMh()
4142  -0.603 * deltaaMZ()
4143  +3.57 * deltaGmu() );
4144 
4145  } else if (Pol_em == 80. && Pol_ep == 0.){
4146  mu +=
4147  +121483. * CHbox / LambdaNP2
4148  +266382. * CHL1_11 / LambdaNP2
4149  -313151. * CHe_11 / LambdaNP2
4150  +245682. * CHL3_11 / LambdaNP2
4151  -168446. * CHD / LambdaNP2
4152  -15072.1 * CHB / LambdaNP2
4153  -6209.98 * CHW / LambdaNP2
4154  -281195. * CHWB / LambdaNP2
4155  +6468.72 * CDHB / LambdaNP2
4156  -7633.09 * CDHW / LambdaNP2
4157  -4.079 * DeltaGF()
4158  -4.832 * deltaMwd6()
4159  ;
4160 
4161  // Add modifications due to small variations of the SM parameters
4162  mu += cHSM * ( +3.758 * deltaMz()
4163  -2.579 * deltaMh()
4164  +0.009 * deltaaMZ()
4165  +2.778 * deltaGmu() );
4166 
4167  } else if (Pol_em == -80. && Pol_ep == 0.){
4168  mu +=
4169  +121500. * CHbox / LambdaNP2
4170  +337280. * CHL1_11 / LambdaNP2
4171  -1209.82 * CHe_11 / LambdaNP2
4172  +283754. * CHL3_11 / LambdaNP2
4173  -199723. * CHD / LambdaNP2
4174  -78465.3 * CHB / LambdaNP2
4175  +34393.4 * CHW / LambdaNP2
4176  -417413. * CHWB / LambdaNP2
4177  -28344.3 * CDHB / LambdaNP2
4178  -1296.23 * CDHW / LambdaNP2
4179  -4.777 * DeltaGF()
4180  -5.539 * deltaMwd6()
4181  ;
4182 
4183  // Add modifications due to small variations of the SM parameters
4184  mu += cHSM * ( +4.99 * deltaMz()
4185  -2.528 * deltaMh()
4186  -0.6 * deltaaMZ()
4187  +3.56 * deltaGmu() );
4188 
4189  } else {
4190  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4191  }
4192 
4193  } else if (sqrt_s == 0.250) {
4194 
4195  C1 = 0.0064;
4196 
4197  if (Pol_em == 80. && Pol_ep == -30.){
4198  mu +=
4199  +120626. * CHbox / LambdaNP2
4200  +172936. * CHL1_11 / LambdaNP2
4201  -516799. * CHe_11 / LambdaNP2
4202  +146366. * CHL3_11 / LambdaNP2
4203  -156275. * CHD / LambdaNP2
4204  +30993.1 * CHB / LambdaNP2
4205  -62277.2 * CHW / LambdaNP2
4206  -213096. * CHWB / LambdaNP2
4207  +32593.7 * CDHB / LambdaNP2
4208  -18479.4 * CDHW / LambdaNP2
4209  -3.678 * DeltaGF()
4210  -4.598 * deltaMwd6()
4211  ;
4212 
4213  // Add modifications due to small variations of the SM parameters
4214  mu += cHSM * ( +2.739 * deltaMz()
4215  -2.661 * deltaMh()
4216  +0.356 * deltaaMZ()
4217  +2.343 * deltaGmu() );
4218 
4219  } else if (Pol_em == -80. && Pol_ep == 30.){
4220  mu +=
4221  +120567. * CHbox / LambdaNP2
4222  +263666. * CHL1_11 / LambdaNP2
4223  -351.165 * CHe_11 / LambdaNP2
4224  -396055. * CHL3_11 / LambdaNP2
4225  -204612. * CHD / LambdaNP2
4226  -64672.8 * CHB / LambdaNP2
4227  -5618.64 * CHW / LambdaNP2
4228  -418629. * CHWB / LambdaNP2
4229  -24815.6 * CDHB / LambdaNP2
4230  -9013.23 * CDHW / LambdaNP2
4231  +286902. * CLL_1221 / LambdaNP2
4232  -5.706 * deltaMwd6()
4233  ;
4234 
4235  // Add modifications due to small variations of the SM parameters
4236  mu += cHSM * ( +4.313 * deltaMz()
4237  -2.793 * deltaMh()
4238  -0.544 * deltaaMZ()
4239  +3.494 * deltaGmu() );
4240 
4241  } else if (Pol_em == 80. && Pol_ep == 0.){
4242  mu +=
4243  +120240. * CHbox / LambdaNP2
4244  +208124. * CHL1_11 / LambdaNP2
4245  -315248. * CHe_11 / LambdaNP2
4246  +158895. * CHL3_11 / LambdaNP2
4247  -175074. * CHD / LambdaNP2
4248  -6529.15 * CHB / LambdaNP2
4249  -40099.4 * CHW / LambdaNP2
4250  -293696. * CHWB / LambdaNP2
4251  +10284.9 * CDHB / LambdaNP2
4252  -15311.7 * CDHW / LambdaNP2
4253  -4.092 * DeltaGF()
4254  -5.01 * deltaMwd6()
4255  ;
4256 
4257  // Add modifications due to small variations of the SM parameters
4258  mu += cHSM * ( +3.351 * deltaMz()
4259  -2.698 * deltaMh()
4260  -0.006 * deltaaMZ()
4261  +2.791 * deltaGmu() );
4262 
4263  } else if (Pol_em == -80. && Pol_ep == 0.){
4264  mu +=
4265  +120459. * CHbox / LambdaNP2
4266  +263262. * CHL1_11 / LambdaNP2
4267  -2507.98 * CHe_11 / LambdaNP2
4268  +177390. * CHL3_11 / LambdaNP2
4269  -204514. * CHD / LambdaNP2
4270  -64371.5 * CHB / LambdaNP2
4271  -5927.95 * CHW / LambdaNP2
4272  -417860. * CHWB / LambdaNP2
4273  -24699.8 * CDHB / LambdaNP2
4274  -9119.93 * CDHW / LambdaNP2
4275  -4.726 * DeltaGF()
4276  -5.715 * deltaMwd6()
4277  ;
4278 
4279  // Add modifications due to small variations of the SM parameters
4280  mu += cHSM * ( +4.305 * deltaMz()
4281  -2.793 * deltaMh()
4282  -0.54 * deltaaMZ()
4283  +3.492 * deltaGmu() );
4284 
4285  } else {
4286  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4287  }
4288 
4289  } else if (sqrt_s == 0.350) {
4290 
4291  C1 = 0.0062;
4292 
4293  if (Pol_em == 80. && Pol_ep == -30.){
4294  mu +=
4295  +120937. * CHbox / LambdaNP2
4296  -41080.7 * CHL1_11 / LambdaNP2
4297  -416801. * CHe_11 / LambdaNP2
4298  -192794. * CHL3_11 / LambdaNP2
4299  -182281. * CHD / LambdaNP2
4300  +102909. * CHB / LambdaNP2
4301  -87947.8 * CHW / LambdaNP2
4302  -228111. * CHWB / LambdaNP2
4303  +40181.7 * CDHB / LambdaNP2
4304  -37530.5 * CDHW / LambdaNP2
4305  -4.236 * DeltaGF()
4306  -4.832 * deltaMwd6()
4307  ;
4308 
4309  // Add modifications due to small variations of the SM parameters
4310  mu += cHSM * ( +3.177 * deltaMz()
4311  -1.894 * deltaMh()
4312  -0.171 * deltaaMZ()
4313  +3.022 * deltaGmu() );
4314 
4315  } else if (Pol_em == -80. && Pol_ep == 30.){
4316  mu +=
4317  +120796. * CHbox / LambdaNP2
4318  -17710.6 * CHL1_11 / LambdaNP2
4319  -1357.61 * CHe_11 / LambdaNP2
4320  -241114. * CHL3_11 / LambdaNP2
4321  -206464. * CHD / LambdaNP2
4322  +5738.97 * CHB / LambdaNP2
4323  -94600.4 * CHW / LambdaNP2
4324  -387581. * CHWB / LambdaNP2
4325  -1403.89 * CDHB / LambdaNP2
4326  -31363.8 * CDHW / LambdaNP2
4327  -4.699 * DeltaGF()
4328  -5.361 * deltaMwd6()
4329  ;
4330 
4331  // Add modifications due to small variations of the SM parameters
4332  mu += cHSM * ( +3.768 * deltaMz()
4333  -2. * deltaMh()
4334  -0.556 * deltaaMZ()
4335  +3.512 * deltaGmu() );
4336 
4337  } else if (Pol_em == 80. && Pol_ep == 0.){
4338  mu +=
4339  +121065. * CHbox / LambdaNP2
4340  -30567.4 * CHL1_11 / LambdaNP2
4341  -235832. * CHe_11 / LambdaNP2
4342  -213581. * CHL3_11 / LambdaNP2
4343  -192620. * CHD / LambdaNP2
4344  +60320.1 * CHB / LambdaNP2
4345  -90446.2 * CHW / LambdaNP2
4346  -297833. * CHWB / LambdaNP2
4347  +22132.1 * CDHB / LambdaNP2
4348  -34844.4 * CDHW / LambdaNP2
4349  -4.439 * DeltaGF()
4350  -5.054 * deltaMwd6()
4351  ;
4352 
4353  // Add modifications due to small variations of the SM parameters
4354  mu += cHSM * ( +3.437 * deltaMz()
4355  -1.943 * deltaMh()
4356  -0.343 * deltaaMZ()
4357  +3.237 * deltaGmu() );
4358 
4359  } else if (Pol_em == -80. && Pol_ep == 0.){
4360  mu +=
4361  +120725. * CHbox / LambdaNP2
4362  -17741.9 * CHL1_11 / LambdaNP2
4363  -2786.58 * CHe_11 / LambdaNP2
4364  -241197. * CHL3_11 / LambdaNP2
4365  -206387. * CHD / LambdaNP2
4366  +6134.48 * CHB / LambdaNP2
4367  -94603.3 * CHW / LambdaNP2
4368  -387053. * CHWB / LambdaNP2
4369  -1323.12 * CDHB / LambdaNP2
4370  -31434.2 * CDHW / LambdaNP2
4371  -4.696 * DeltaGF()
4372  -5.365 * deltaMwd6()
4373  ;
4374 
4375  // Add modifications due to small variations of the SM parameters
4376  mu += cHSM * ( +3.764 * deltaMz()
4377  -2. * deltaMh()
4378  -0.556 * deltaaMZ()
4379  +3.517 * deltaGmu() );
4380 
4381  } else {
4382  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4383  }
4384 
4385  } else if (sqrt_s == 0.365) {
4386 
4387  C1 = 0.0062; // Use the same as 350 GeV
4388 
4389  if (Pol_em == 80. && Pol_ep == -30.){
4390  mu +=
4391  +121120. * CHbox / LambdaNP2
4392  -43274.8 * CHL1_11 / LambdaNP2
4393  -379332. * CHe_11 / LambdaNP2
4394  -213151. * CHL3_11 / LambdaNP2
4395  -185704. * CHD / LambdaNP2
4396  +95027.9 * CHB / LambdaNP2
4397  -87042.2 * CHW / LambdaNP2
4398  -246839. * CHWB / LambdaNP2
4399  +37834.6 * CDHB / LambdaNP2
4400  -38594.2 * CDHW / LambdaNP2
4401  -4.314 * DeltaGF()
4402  -4.867 * deltaMwd6()
4403  ;
4404 
4405  // Add modifications due to small variations of the SM parameters
4406  mu += cHSM * ( +3.356 * deltaMz()
4407  -1.787 * deltaMh()
4408  -0.246 * deltaaMZ()
4409  +3.12 * deltaGmu() );
4410 
4411  } else if (Pol_em == -80. && Pol_ep == 30.){
4412  mu +=
4413  +120708. * CHbox / LambdaNP2
4414  -23163.4 * CHL1_11 / LambdaNP2
4415  -1266.64 * CHe_11 / LambdaNP2
4416  -256145. * CHL3_11 / LambdaNP2
4417  -206112. * CHD / LambdaNP2
4418  +7209.08 * CHB / LambdaNP2
4419  -94095.3 * CHW / LambdaNP2
4420  -386056. * CHWB / LambdaNP2
4421  -673.745 * CDHB / LambdaNP2
4422  -32528.4 * CDHW / LambdaNP2
4423  -4.703 * DeltaGF()
4424  -5.297 * deltaMwd6()
4425  ;
4426 
4427  // Add modifications due to small variations of the SM parameters
4428  mu += cHSM * ( +3.865 * deltaMz()
4429  -1.869 * deltaMh()
4430  -0.577 * deltaaMZ()
4431  +3.533 * deltaGmu() );
4432 
4433  } else if (Pol_em == 80. && Pol_ep == 0.){
4434  mu +=
4435  +120872. * CHbox / LambdaNP2
4436  -34492.1 * CHL1_11 / LambdaNP2
4437  -212361. * CHe_11 / LambdaNP2
4438  -232050. * CHL3_11 / LambdaNP2
4439  -194801. * CHD / LambdaNP2
4440  +56353. * CHB / LambdaNP2
4441  -90080.9 * CHW / LambdaNP2
4442  -308151. * CHWB / LambdaNP2
4443  +20707.2 * CDHB / LambdaNP2
4444  -35840.6 * CDHW / LambdaNP2
4445  -4.485 * DeltaGF()
4446  -5.033 * deltaMwd6()
4447  ;
4448 
4449  // Add modifications due to small variations of the SM parameters
4450  mu += cHSM * ( +3.586 * deltaMz()
4451  -1.817 * deltaMh()
4452  -0.393 * deltaaMZ()
4453  +3.287 * deltaGmu() );
4454 
4455  } else if (Pol_em == -80. && Pol_ep == 0.){
4456  mu +=
4457  +120806. * CHbox / LambdaNP2
4458  -23082.3 * CHL1_11 / LambdaNP2
4459  -2521.89 * CHe_11 / LambdaNP2
4460  -255807. * CHL3_11 / LambdaNP2
4461  -205972. * CHD / LambdaNP2
4462  +7600.7 * CHB / LambdaNP2
4463  -94080.6 * CHW / LambdaNP2
4464  -385587. * CHWB / LambdaNP2
4465  -525.394 * CDHB / LambdaNP2
4466  -32486.9 * CDHW / LambdaNP2
4467  -4.703 * DeltaGF()
4468  -5.294 * deltaMwd6()
4469  ;
4470 
4471  // Add modifications due to small variations of the SM parameters
4472  mu += cHSM * ( +3.87 * deltaMz()
4473  -1.873 * deltaMh()
4474  -0.577 * deltaaMZ()
4475  +3.533 * deltaGmu() );
4476 
4477  } else {
4478  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4479  }
4480 
4481  } else if (sqrt_s == 0.380) {
4482 
4483  C1 = 0.0062; // Use the same as 350 GeV
4484 
4485  if (Pol_em == 80. && Pol_ep == -30.){
4486  mu +=
4487  +120907. * CHbox / LambdaNP2
4488  -43917.7 * CHL1_11 / LambdaNP2
4489  -344628. * CHe_11 / LambdaNP2
4490  -230932. * CHL3_11 / LambdaNP2
4491  -188656. * CHD / LambdaNP2
4492  +86802.5 * CHB / LambdaNP2
4493  -86378.3 * CHW / LambdaNP2
4494  -262732. * CHWB / LambdaNP2
4495  +35211.7 * CDHB / LambdaNP2
4496  -39122. * CDHW / LambdaNP2
4497  -4.375 * DeltaGF()
4498  -4.833 * deltaMwd6()
4499  ;
4500 
4501  // Add modifications due to small variations of the SM parameters
4502  mu += cHSM * ( +3.526 * deltaMz()
4503  -1.675 * deltaMh()
4504  -0.322 * deltaaMZ()
4505  +3.202 * deltaGmu() );
4506 
4507  } else if (Pol_em == -80. && Pol_ep == 30.){
4508  mu +=
4509  +120826. * CHbox / LambdaNP2
4510  -26397.1 * CHL1_11 / LambdaNP2
4511  -1156.51 * CHe_11 / LambdaNP2
4512  -268680. * CHL3_11 / LambdaNP2
4513  -205752. * CHD / LambdaNP2
4514  +8226.72 * CHB / LambdaNP2
4515  -92973.9 * CHW / LambdaNP2
4516  -384868. * CHWB / LambdaNP2
4517  -154.996 * CDHB / LambdaNP2
4518  -33479.2 * CDHW / LambdaNP2
4519  -4.706 * DeltaGF()
4520  -5.24 * deltaMwd6()
4521  ;
4522 
4523  // Add modifications due to small variations of the SM parameters
4524  mu += cHSM * ( +3.957 * deltaMz()
4525  -1.756 * deltaMh()
4526  -0.592 * deltaaMZ()
4527  +3.551 * deltaGmu() );
4528 
4529  } else if (Pol_em == 80. && Pol_ep == 0.){
4530  mu +=
4531  +121123. * CHbox / LambdaNP2
4532  -35934.5 * CHL1_11 / LambdaNP2
4533  -191922. * CHe_11 / LambdaNP2
4534  -247636. * CHL3_11 / LambdaNP2
4535  -196255. * CHD / LambdaNP2
4536  +52143.1 * CHB / LambdaNP2
4537  -89227.7 * CHW / LambdaNP2
4538  -317018. * CHWB / LambdaNP2
4539  +19725.8 * CDHB / LambdaNP2
4540  -36723.5 * CDHW / LambdaNP2
4541  -4.524 * DeltaGF()
4542  -5.007 * deltaMwd6()
4543  ;
4544 
4545  // Add modifications due to small variations of the SM parameters
4546  mu += cHSM * ( +3.729 * deltaMz()
4547  -1.706 * deltaMh()
4548  -0.439 * deltaaMZ()
4549  +3.366 * deltaGmu() );
4550 
4551  } else if (Pol_em == -80. && Pol_ep == 0.){
4552  mu +=
4553  +120839. * CHbox / LambdaNP2
4554  -26545. * CHL1_11 / LambdaNP2
4555  -2293.44 * CHe_11 / LambdaNP2
4556  -268673. * CHL3_11 / LambdaNP2
4557  -205696. * CHD / LambdaNP2
4558  +8476.41 * CHB / LambdaNP2
4559  -92899.6 * CHW / LambdaNP2
4560  -384414. * CHWB / LambdaNP2
4561  +15.496 * CDHB / LambdaNP2
4562  -33502.8 * CDHW / LambdaNP2
4563  -4.704 * DeltaGF()
4564  -5.232 * deltaMwd6()
4565  ;
4566 
4567  // Add modifications due to small variations of the SM parameters
4568  mu += cHSM * ( +3.958 * deltaMz()
4569  -1.755 * deltaMh()
4570  -0.59 * deltaaMZ()
4571  +3.555 * deltaGmu() );
4572 
4573  } else {
4574  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4575  }
4576 
4577  } else if (sqrt_s == 0.500) {
4578 
4579  C1 = 0.0061;
4580 
4581  if (Pol_em == 80. && Pol_ep == -30.){
4582  mu +=
4583  +120734. * CHbox / LambdaNP2
4584  -33626. * CHL1_11 / LambdaNP2
4585  -177471. * CHe_11 / LambdaNP2
4586  -312922. * CHL3_11 / LambdaNP2
4587  -199388. * CHD / LambdaNP2
4588  +44288.8 * CHB / LambdaNP2
4589  -78960.3 * CHW / LambdaNP2
4590  -332501. * CHWB / LambdaNP2
4591  +20615.5 * CDHB / LambdaNP2
4592  -43923.9 * CDHW / LambdaNP2
4593  -4.614 * DeltaGF()
4594  -4.84 * deltaMwd6()
4595  ;
4596 
4597  // Add modifications due to small variations of the SM parameters
4598  mu += cHSM * ( +4.296 * deltaMz()
4599  -1.178 * deltaMh()
4600  -0.582 * deltaaMZ()
4601  +3.535 * deltaGmu() );
4602 
4603  } else if (Pol_em == -80. && Pol_ep == 30.){
4604  mu +=
4605  +120746. * CHbox / LambdaNP2
4606  -26369.8 * CHL1_11 / LambdaNP2
4607  -905.141 * CHe_11 / LambdaNP2
4608  -327709. * CHL3_11 / LambdaNP2
4609  -204622. * CHD / LambdaNP2
4610  +8508.33 * CHB / LambdaNP2
4611  -82669.6 * CHW / LambdaNP2
4612  -381185. * CHWB / LambdaNP2
4613  +784.456 * CDHB / LambdaNP2
4614  -41153.8 * CDHW / LambdaNP2
4615  -4.711 * DeltaGF()
4616  -4.948 * deltaMwd6()
4617  ;
4618 
4619  // Add modifications due to small variations of the SM parameters
4620  mu += cHSM * ( +4.417 * deltaMz()
4621  -1.196 * deltaMh()
4622  -0.664 * deltaaMZ()
4623  +3.639 * deltaGmu() );
4624 
4625  } else if (Pol_em == 80. && Pol_ep == 0.){
4626  mu +=
4627  +120667. * CHbox / LambdaNP2
4628  -30480.6 * CHL1_11 / LambdaNP2
4629  -96672.9 * CHe_11 / LambdaNP2
4630  -320011. * CHL3_11 / LambdaNP2
4631  -201855. * CHD / LambdaNP2
4632  +27690.6 * CHB / LambdaNP2
4633  -80770. * CHW / LambdaNP2
4634  -355060. * CHWB / LambdaNP2
4635  +11299.4 * CDHB / LambdaNP2
4636  -42756.5 * CDHW / LambdaNP2
4637  -4.656 * DeltaGF()
4638  -4.875 * deltaMwd6()
4639  ;
4640 
4641  // Add modifications due to small variations of the SM parameters
4642  mu += cHSM * ( +4.345 * deltaMz()
4643  -1.186 * deltaMh()
4644  -0.621 * deltaaMZ()
4645  +3.589 * deltaGmu() );
4646 
4647  } else if (Pol_em == -80. && Pol_ep == 0.){
4648  mu +=
4649  +120715. * CHbox / LambdaNP2
4650  -26433.4 * CHL1_11 / LambdaNP2
4651  -1490.31 * CHe_11 / LambdaNP2
4652  -327665. * CHL3_11 / LambdaNP2
4653  -204644. * CHD / LambdaNP2
4654  +8471.25 * CHB / LambdaNP2
4655  -82673.2 * CHW / LambdaNP2
4656  -381049. * CHWB / LambdaNP2
4657  +862.813 * CDHB / LambdaNP2
4658  -41179.7 * CDHW / LambdaNP2
4659  -4.711 * DeltaGF()
4660  -4.942 * deltaMwd6()
4661  ;
4662 
4663  // Add modifications due to small variations of the SM parameters
4664  mu += cHSM * ( +4.416 * deltaMz()
4665  -1.194 * deltaMh()
4666  -0.664 * deltaaMZ()
4667  +3.64 * deltaGmu() );
4668 
4669  } else {
4670  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4671  }
4672 
4673  } else if (sqrt_s == 1.0) {
4674 
4675  C1 = 0.0059;
4676 
4677  if (Pol_em == 80. && Pol_ep == -30.){
4678  mu +=
4679  +120494. * CHbox / LambdaNP2
4680  -9728.66 * CHL1_11 / LambdaNP2
4681  -46166.9 * CHe_11 / LambdaNP2
4682  -452752. * CHL3_11 / LambdaNP2
4683  -203700. * CHD / LambdaNP2
4684  +8561.22 * CHB / LambdaNP2
4685  -61449.7 * CHW / LambdaNP2
4686  -374076. * CHWB / LambdaNP2
4687  +6473.98 * CDHB / LambdaNP2
4688  -64032.3 * CDHW / LambdaNP2
4689  -4.706 * DeltaGF()
4690  -4.581 * deltaMwd6()
4691  ;
4692 
4693  // Add modifications due to small variations of the SM parameters
4694  mu += cHSM * ( +4.956 * deltaMz()
4695  -0.583 * deltaMh()
4696  -0.739 * deltaaMZ()
4697  +3.723 * deltaGmu() );
4698 
4699  } else if (Pol_em == -80. && Pol_ep == 30.){
4700  mu +=
4701  +120522. * CHbox / LambdaNP2
4702  -8881.26 * CHL1_11 / LambdaNP2
4703  -529.908 * CHe_11 / LambdaNP2
4704  -454326. * CHL3_11 / LambdaNP2
4705  -204057. * CHD / LambdaNP2
4706  +3158.25 * CHB / LambdaNP2
4707  -61850.9 * CHW / LambdaNP2
4708  -380114. * CHWB / LambdaNP2
4709  +63.589 * CDHB / LambdaNP2
4710  -63800.9 * CDHW / LambdaNP2
4711  -4.712 * DeltaGF()
4712  -4.587 * deltaMwd6()
4713  ;
4714 
4715  // Add modifications due to small variations of the SM parameters
4716  mu += cHSM * ( +4.967 * deltaMz()
4717  -0.582 * deltaMh()
4718  -0.746 * deltaaMZ()
4719  +3.731 * deltaGmu() );
4720 
4721  } else if (Pol_em == 80. && Pol_ep == 0.){
4722  mu +=
4723  +120509. * CHbox / LambdaNP2
4724  -9342.32 * CHL1_11 / LambdaNP2
4725  -25028.5 * CHe_11 / LambdaNP2
4726  -453487. * CHL3_11 / LambdaNP2
4727  -203871. * CHD / LambdaNP2
4728  +6021.71 * CHB / LambdaNP2
4729  -61580. * CHW / LambdaNP2
4730  -376790. * CHWB / LambdaNP2
4731  +3494.08 * CDHB / LambdaNP2
4732  -63959. * CDHW / LambdaNP2
4733  -4.708 * DeltaGF()
4734  -4.589 * deltaMwd6()
4735  ;
4736 
4737  // Add modifications due to small variations of the SM parameters
4738  mu += cHSM * ( +4.962 * deltaMz()
4739  -0.582 * deltaMh()
4740  -0.742 * deltaaMZ()
4741  +3.726 * deltaGmu() );
4742 
4743  } else if (Pol_em == -80. && Pol_ep == 0.){
4744  mu +=
4745  +120526. * CHbox / LambdaNP2
4746  -8927.83 * CHL1_11 / LambdaNP2
4747  -633.766 * CHe_11 / LambdaNP2
4748  -454337. * CHL3_11 / LambdaNP2
4749  -204073. * CHD / LambdaNP2
4750  +3196.39 * CHB / LambdaNP2
4751  -61833.5 * CHW / LambdaNP2
4752  -380094. * CHWB / LambdaNP2
4753  +82.665 * CDHB / LambdaNP2
4754  -63817.5 * CDHW / LambdaNP2
4755  -4.712 * DeltaGF()
4756  -4.588 * deltaMwd6()
4757  ;
4758 
4759  // Add modifications due to small variations of the SM parameters
4760  mu += cHSM * ( +4.967 * deltaMz()
4761  -0.582 * deltaMh()
4762  -0.746 * deltaaMZ()
4763  +3.731 * deltaGmu() );
4764 
4765  } else {
4766  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4767  }
4768 
4769  } else if (sqrt_s == 1.4) {
4770 
4771  C1 = 0.0058;
4772 
4773  if (Pol_em == 80. && Pol_ep == -30.){
4774  mu +=
4775  +120516. * CHbox / LambdaNP2
4776  -5019.36 * CHL1_11 / LambdaNP2
4777  -29937.8 * CHe_11 / LambdaNP2
4778  -521211. * CHL3_11 / LambdaNP2
4779  -203908. * CHD / LambdaNP2
4780  +4153.08 * CHB / LambdaNP2
4781  -54219.3 * CHW / LambdaNP2
4782  -377548. * CHWB / LambdaNP2
4783  +4509.78 * CDHB / LambdaNP2
4784  -76054.8 * CDHW / LambdaNP2
4785  -4.71 * DeltaGF()
4786  -4.484 * deltaMwd6()
4787  ;
4788 
4789  // Add modifications due to small variations of the SM parameters
4790  mu += cHSM * ( +5.105 * deltaMz()
4791  -0.447 * deltaMh()
4792  -0.765 * deltaaMZ()
4793  +3.747 * deltaGmu() );
4794 
4795  } else if (Pol_em == -80. && Pol_ep == 30.){
4796  mu +=
4797  +120530. * CHbox / LambdaNP2
4798  -4727.84 * CHL1_11 / LambdaNP2
4799  -488.036 * CHe_11 / LambdaNP2
4800  -521821. * CHL3_11 / LambdaNP2
4801  -204045. * CHD / LambdaNP2
4802  +1784.38 * CHB / LambdaNP2
4803  -54507.5 * CHW / LambdaNP2
4804  -380042. * CHWB / LambdaNP2
4805  -122.009 * CDHB / LambdaNP2
4806  -75950.5 * CDHW / LambdaNP2
4807  -4.712 * DeltaGF()
4808  -4.487 * deltaMwd6()
4809  ;
4810 
4811  // Add modifications due to small variations of the SM parameters
4812  mu += cHSM * ( +5.108 * deltaMz()
4813  -0.447 * deltaMh()
4814  -0.768 * deltaaMZ()
4815  +3.749 * deltaGmu() );
4816 
4817  } else if (Pol_em == 80. && Pol_ep == 0.){
4818  mu +=
4819  +120542. * CHbox / LambdaNP2
4820  -4870.22 * CHL1_11 / LambdaNP2
4821  -16376.8 * CHe_11 / LambdaNP2
4822  -521472. * CHL3_11 / LambdaNP2
4823  -203960. * CHD / LambdaNP2
4824  +3068.42 * CHB / LambdaNP2
4825  -54375.2 * CHW / LambdaNP2
4826  -378699. * CHWB / LambdaNP2
4827  +2390.51 * CDHB / LambdaNP2
4828  -75996.8 * CDHW / LambdaNP2
4829  -4.711 * DeltaGF()
4830  -4.485 * deltaMwd6()
4831  ;
4832 
4833  // Add modifications due to small variations of the SM parameters
4834  mu += cHSM * ( +5.107 * deltaMz()
4835  -0.448 * deltaMh()
4836  -0.766 * deltaaMZ()
4837  +3.749 * deltaGmu() );
4838 
4839  } else if (Pol_em == -80. && Pol_ep == 0.){
4840  mu +=
4841  +120504. * CHbox / LambdaNP2
4842  -4718.66 * CHL1_11 / LambdaNP2
4843  -574.963 * CHe_11 / LambdaNP2
4844  -521805. * CHL3_11 / LambdaNP2
4845  -204053. * CHD / LambdaNP2
4846  +1784.37 * CHB / LambdaNP2
4847  -54482.7 * CHW / LambdaNP2
4848  -380051. * CHWB / LambdaNP2
4849  -99.132 * CDHB / LambdaNP2
4850  -75974.5 * CDHW / LambdaNP2
4851  -4.712 * DeltaGF()
4852  -4.487 * deltaMwd6()
4853  ;
4854 
4855  // Add modifications due to small variations of the SM parameters
4856  mu += cHSM * ( +5.107 * deltaMz()
4857  -0.447 * deltaMh()
4858  -0.767 * deltaaMZ()
4859  +3.749 * deltaGmu() );
4860 
4861  } else {
4862  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4863  }
4864 
4865  } else if (sqrt_s == 1.5) {
4866 
4867  C1 = 0.0058;// Use the same as 1400 GeV
4868 
4869  if (Pol_em == 80. && Pol_ep == -30.){
4870  mu +=
4871  +120531. * CHbox / LambdaNP2
4872  -4421.38 * CHL1_11 / LambdaNP2
4873  -28114.2 * CHe_11 / LambdaNP2
4874  -535633. * CHL3_11 / LambdaNP2
4875  -203960. * CHD / LambdaNP2
4876  +3556.32 * CHB / LambdaNP2
4877  -52816.2 * CHW / LambdaNP2
4878  -377932. * CHWB / LambdaNP2
4879  +4253.17 * CDHB / LambdaNP2
4880  -78599.6 * CDHW / LambdaNP2
4881  -4.71 * DeltaGF()
4882  -4.465 * deltaMwd6()
4883  ;
4884 
4885  // Add modifications due to small variations of the SM parameters
4886  mu += cHSM * ( +5.128 * deltaMz()
4887  -0.424 * deltaMh()
4888  -0.772 * deltaaMZ()
4889  +3.755 * deltaGmu() );
4890 
4891  } else if (Pol_em == -80. && Pol_ep == 30.){
4892  mu +=
4893  +120491. * CHbox / LambdaNP2
4894  -4113.21 * CHL1_11 / LambdaNP2
4895  -517.747 * CHe_11 / LambdaNP2
4896  -536169. * CHL3_11 / LambdaNP2
4897  -204050. * CHD / LambdaNP2
4898  +1553.24 * CHB / LambdaNP2
4899  -53097.9 * CHW / LambdaNP2
4900  -380055. * CHWB / LambdaNP2
4901  -129.437 * CDHB / LambdaNP2
4902  -78539.4 * CDHW / LambdaNP2
4903  -4.711 * DeltaGF()
4904  -4.468 * deltaMwd6()
4905  ;
4906 
4907  // Add modifications due to small variations of the SM parameters
4908  mu += cHSM * ( +5.131 * deltaMz()
4909  -0.424 * deltaMh()
4910  -0.773 * deltaaMZ()
4911  +3.755 * deltaGmu() );
4912 
4913  } else if (Pol_em == 80. && Pol_ep == 0.){
4914  mu +=
4915  +120525. * CHbox / LambdaNP2
4916  -4256.39 * CHL1_11 / LambdaNP2
4917  -15376.9 * CHe_11 / LambdaNP2
4918  -535845. * CHL3_11 / LambdaNP2
4919  -203987. * CHD / LambdaNP2
4920  +2641.32 * CHB / LambdaNP2
4921  -53045.1 * CHW / LambdaNP2
4922  -378920. * CHWB / LambdaNP2
4923  +2237.55 * CDHB / LambdaNP2
4924  -78549.8 * CDHW / LambdaNP2
4925  -4.711 * DeltaGF()
4926  -4.468 * deltaMwd6()
4927  ;
4928 
4929  // Add modifications due to small variations of the SM parameters
4930  mu += cHSM * ( +5.129 * deltaMz()
4931  -0.424 * deltaMh()
4932  -0.772 * deltaaMZ()
4933  +3.753 * deltaGmu() );
4934 
4935  } else if (Pol_em == -80. && Pol_ep == 0.){
4936  mu +=
4937  +120499. * CHbox / LambdaNP2
4938  -4113.23 * CHL1_11 / LambdaNP2
4939  -616.984 * CHe_11 / LambdaNP2
4940  -536155. * CHL3_11 / LambdaNP2
4941  -204035. * CHD / LambdaNP2
4942  +1570.5 * CHB / LambdaNP2
4943  -53079.3 * CHW / LambdaNP2
4944  -380043. * CHWB / LambdaNP2
4945  -112.179 * CDHB / LambdaNP2
4946  -78543.9 * CDHW / LambdaNP2
4947  -4.711 * DeltaGF()
4948  -4.468 * deltaMwd6()
4949  ;
4950 
4951  // Add modifications due to small variations of the SM parameters
4952  mu += cHSM * ( +5.13 * deltaMz()
4953  -0.424 * deltaMh()
4954  -0.773 * deltaaMZ()
4955  +3.755 * deltaGmu() );
4956 
4957  } else {
4958  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4959  }
4960 
4961  } else if (sqrt_s == 3.0) {
4962 
4963  C1 = 0.0057;
4964 
4965  if (Pol_em == 80. && Pol_ep == -30.){
4966  mu +=
4967  +120384. * CHbox / LambdaNP2
4968  -1301.85 * CHL1_11 / LambdaNP2
4969  -16370.4 * CHe_11 / LambdaNP2
4970  -686389. * CHL3_11 / LambdaNP2
4971  -204031. * CHD / LambdaNP2
4972  +628.479 * CHB / LambdaNP2
4973  -41464.7 * CHW / LambdaNP2
4974  -379766. * CHWB / LambdaNP2
4975  +2259.53 * CDHB / LambdaNP2
4976  -104941. * CDHW / LambdaNP2
4977  -4.706 * DeltaGF()
4978  -4.342 * deltaMwd6()
4979  ;
4980 
4981  // Add modifications due to small variations of the SM parameters
4982  mu += cHSM * ( +5.306 * deltaMz()
4983  -0.283 * deltaMh()
4984  -0.802 * deltaaMZ()
4985  +3.787 * deltaGmu() );
4986 
4987  } else if (Pol_em == -80. && Pol_ep == 30.){
4988  mu +=
4989  +120423. * CHbox / LambdaNP2
4990  -1253.47 * CHL1_11 / LambdaNP2
4991  -537.201 * CHe_11 / LambdaNP2
4992  -686427. * CHL3_11 / LambdaNP2
4993  -204047. * CHD / LambdaNP2
4994  +268.601 * CHB / LambdaNP2
4995  -41454. * CHW / LambdaNP2
4996  -380141. * CHWB / LambdaNP2
4997  -447.668 * CDHB / LambdaNP2
4998  -104906. * CDHW / LambdaNP2
4999  -4.707 * DeltaGF()
5000  -4.342 * deltaMwd6()
5001  ;
5002 
5003  // Add modifications due to small variations of the SM parameters
5004  mu += cHSM * ( +5.305 * deltaMz()
5005  -0.284 * deltaMh()
5006  -0.802 * deltaaMZ()
5007  +3.787 * deltaGmu() );
5008 
5009  } else if (Pol_em == 80. && Pol_ep == 0.){
5010  mu +=
5011  +120399. * CHbox / LambdaNP2
5012  -1267.47 * CHL1_11 / LambdaNP2
5013  -9008.44 * CHe_11 / LambdaNP2
5014  -686485. * CHL3_11 / LambdaNP2
5015  -204052. * CHD / LambdaNP2
5016  +439.947 * CHB / LambdaNP2
5017  -41459.8 * CHW / LambdaNP2
5018  -379947. * CHWB / LambdaNP2
5019  +1005.59 * CDHB / LambdaNP2
5020  -104927. * CDHW / LambdaNP2
5021  -4.706 * DeltaGF()
5022  -4.342 * deltaMwd6()
5023  ;
5024 
5025  // Add modifications due to small variations of the SM parameters
5026  mu += cHSM * ( +5.303 * deltaMz()
5027  -0.283 * deltaMh()
5028  -0.802 * deltaaMZ()
5029  +3.789 * deltaGmu() );
5030 
5031  } else if (Pol_em == -80. && Pol_ep == 0.){
5032  mu +=
5033  +120385. * CHbox / LambdaNP2
5034  -1245.4 * CHL1_11 / LambdaNP2
5035  -535.407 * CHe_11 / LambdaNP2
5036  -686461. * CHL3_11 / LambdaNP2
5037  -204048. * CHD / LambdaNP2
5038  +244.425 * CHB / LambdaNP2
5039  -41447.5 * CHW / LambdaNP2
5040  -380150. * CHWB / LambdaNP2
5041  -430.653 * CDHB / LambdaNP2
5042  -104905. * CDHW / LambdaNP2
5043  -4.706 * DeltaGF()
5044  -4.343 * deltaMwd6()
5045  ;
5046 
5047  // Add modifications due to small variations of the SM parameters
5048  mu += cHSM * ( +5.307 * deltaMz()
5049  -0.283 * deltaMh()
5050  -0.802 * deltaaMZ()
5051  +3.789 * deltaGmu() );
5052 
5053  } else {
5054  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5055  }
5056 
5057  } else
5058  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5059 
5060  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5061  mu += eeeWBFint + eeeWBFpar;
5062 
5063 // Linear contribution from Higgs self-coupling
5064  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5065 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5067 
5068  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5069 
5070  return mu;
5071 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CLL_1221
Definition: NPSMEFTd6.h:3592
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueettH()

double NPSMEFTd6::mueettH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 8422 of file NPSMEFTd6.cpp.

8423 {
8424  double mu = 1.0;
8425 
8426  double C1 = 0.0;
8427 
8428  if (sqrt_s == 0.500) {
8429 
8430  C1 = 0.086;
8431 
8432  mu +=
8433  +121901. * CHbox / LambdaNP2
8434  +84038.2 * CHL1_11 / LambdaNP2
8435  +41671.2 * CHe_11 / LambdaNP2
8436  -31418.2 * CHu_11 / LambdaNP2
8437  +84038.2 * CHL3_11 / LambdaNP2
8438  -121791. * CuH_33r / LambdaNP2
8439  -59467.6 * CHD / LambdaNP2
8440  +138929. * CHB / LambdaNP2
8441  +130909. * CHW / LambdaNP2
8442  -253030. * CHWB / LambdaNP2
8443  -1757.66 * CDHB / LambdaNP2
8444  +1501.34 * CDHW / LambdaNP2
8445  +1386027. * CuW_33r / LambdaNP2
8446  +1698012. * CuB_33r / LambdaNP2
8447  -1.965 * DeltaGF()
8448  -1.187 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8449  ;
8450 
8451  // Add modifications due to small variations of the SM parameters
8452  mu += cHSM * ( +1.932 * deltaMz()
8453  -9.827 * deltaMh()
8454  +1.04 * deltaaMZ()
8455  +1.992 * deltaGmu()
8456  -18.476 * deltamt() );
8457 
8458  if (FlagQuadraticTerms) {
8459  //Add contributions that are quadratic in the effective coefficients
8460  mu += 0.0;
8461  }
8462 
8463  } else if (sqrt_s == 1.0) {
8464 
8465  C1 = 0.017;
8466 
8467  mu +=
8468  +122013. * CHbox / LambdaNP2
8469  +889282. * CHL1_11 / LambdaNP2
8470  -543424. * CHe_11 / LambdaNP2
8471  -8240.83 * CHu_11 / LambdaNP2
8472  +889282. * CHL3_11 / LambdaNP2
8473  -116099. * CuH_33r / LambdaNP2
8474  -60351.9 * CHD / LambdaNP2
8475  +352804. * CHB / LambdaNP2
8476  +361918. * CHW / LambdaNP2
8477  -397547. * CHWB / LambdaNP2
8478  +37326.1 * CDHB / LambdaNP2
8479  +113772. * CDHW / LambdaNP2
8480  +2758980. * CuW_33r / LambdaNP2
8481  +3462941. * CuB_33r / LambdaNP2
8482  -2.08 * DeltaGF()
8483  -2.575 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8484  ;
8485 
8486  // Add modifications due to small variations of the SM parameters
8487  mu += cHSM * ( +2.185 * deltaMz()
8488  -1.195 * deltaMh()
8489  +0.92 * deltaaMZ()
8490  +2.096 * deltaGmu()
8491  +2.136 * deltamt() );
8492 
8493  if (FlagQuadraticTerms) {
8494  //Add contributions that are quadratic in the effective coefficients
8495  mu += 0.0;
8496  }
8497 
8498  } else if (sqrt_s == 1.4) {
8499 
8500  C1 = 0.0094;
8501 
8502  mu +=
8503  +122081. * CHbox / LambdaNP2
8504  +2544832. * CHL1_11 / LambdaNP2
8505  -1901938. * CHe_11 / LambdaNP2
8506  +3241.73 * CHu_11 / LambdaNP2
8507  +2544832. * CHL3_11 / LambdaNP2
8508  -112208. * CuH_33r / LambdaNP2
8509  -60340.4 * CHD / LambdaNP2
8510  +464967. * CHB / LambdaNP2
8511  +487659. * CHW / LambdaNP2
8512  -471053. * CHWB / LambdaNP2
8513  +134900. * CDHB / LambdaNP2
8514  +371767. * CDHW / LambdaNP2
8515  +3804096. * CuW_33r / LambdaNP2
8516  +4800265. * CuB_33r / LambdaNP2
8517  -2.139 * DeltaGF()
8518  -3.203 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8519  ;
8520 
8521  // Add modifications due to small variations of the SM parameters
8522  mu += cHSM * ( +2.309 * deltaMz()
8523  -0.898 * deltaMh()
8524  +0.872 * deltaaMZ()
8525  +2.157 * deltaGmu()
8526  +2.262 * deltamt() );
8527 
8528  if (FlagQuadraticTerms) {
8529  //Add contributions that are quadratic in the effective coefficients
8530  mu += 0.0;
8531  }
8532 
8533  } else if (sqrt_s == 1.5) {
8534 
8535  C1 = 0.0094;// Use the same as 1400 GeV
8536 
8537  mu +=
8538  +122173. * CHbox / LambdaNP2
8539  +3117293. * CHL1_11 / LambdaNP2
8540  -2378233. * CHe_11 / LambdaNP2
8541  +5531.15 * CHu_11 / LambdaNP2
8542  +3117293. * CHL3_11 / LambdaNP2
8543  -111274. * CuH_33r / LambdaNP2
8544  -60192. * CHD / LambdaNP2
8545  +487962. * CHB / LambdaNP2
8546  +513503. * CHW / LambdaNP2
8547  -485782. * CHWB / LambdaNP2
8548  +170734. * CDHB / LambdaNP2
8549  +462665. * CDHW / LambdaNP2
8550  +4068326. * CuW_33r / LambdaNP2
8551  +5138930. * CuB_33r / LambdaNP2
8552  -2.149 * DeltaGF()
8553  -3.325 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8554  ;
8555 
8556  // Add modifications due to small variations of the SM parameters
8557  mu += cHSM * ( +2.322 * deltaMz()
8558  -0.858 * deltaMh()
8559  +0.866 * deltaaMZ()
8560  +2.164 * deltaGmu()
8561  +2.265 * deltamt() );
8562 
8563  if (FlagQuadraticTerms) {
8564  //Add contributions that are quadratic in the effective coefficients
8565  mu += 0.0;
8566  }
8567 
8568  } else if (sqrt_s == 3.0) {
8569 
8570  C1 = 0.0037;
8571 
8572  mu +=
8573  +121915. * CHbox / LambdaNP2
8574  +19529668. * CHL1_11 / LambdaNP2
8575  -16356276. * CHe_11 / LambdaNP2
8576  +23142.9 * CHu_11 / LambdaNP2
8577  +19529668. * CHL3_11 / LambdaNP2
8578  -104011. * CuH_33r / LambdaNP2
8579  -58710.4 * CHD / LambdaNP2
8580  +697868. * CHB / LambdaNP2
8581  +751003. * CHW / LambdaNP2
8582  -625171. * CHWB / LambdaNP2
8583  +1204441. * CDHB / LambdaNP2
8584  +3111413. * CDHW / LambdaNP2
8585  +8604912. * CuW_33r / LambdaNP2
8586  +10946841. * CuB_33r / LambdaNP2
8587  -2.224 * DeltaGF()
8588  -4.279 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8589  ;
8590 
8591  // Add modifications due to small variations of the SM parameters
8592  mu += cHSM * ( +2.483 * deltaMz()
8593  -0.572 * deltaMh()
8594  +0.771 * deltaaMZ()
8595  +2.242 * deltaGmu()
8596  +2.182 * deltamt() );
8597 
8598  if (FlagQuadraticTerms) {
8599  //Add contributions that are quadratic in the effective coefficients
8600  mu += 0.0;
8601  }
8602 
8603  } else
8604  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettH()");
8605 
8606  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8607  mu += eeettHint + eeettHpar;
8608 
8609 // Linear contribution from Higgs self-coupling
8610  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8611 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8613 
8614  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8615 
8616  return mu;
8617 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3650
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3651
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ mueettHPol()

double NPSMEFTd6::mueettHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 8619 of file NPSMEFTd6.cpp.

8620 {
8621  double mu = 1.0;
8622 
8623  double C1 = 0.0;
8624 
8625  if (sqrt_s == 0.500) {
8626 
8627  C1 = 0.086;
8628 
8629  if (Pol_em == 80. && Pol_ep == -30.){
8630  mu +=
8631  +121861. * CHbox / LambdaNP2
8632  +14207.9 * CHL1_11 / LambdaNP2
8633  +124191. * CHe_11 / LambdaNP2
8634  +112591. * CHu_11 / LambdaNP2
8635  +14207.9 * CHL3_11 / LambdaNP2
8636  -123399. * CuH_33r / LambdaNP2
8637  -12437.7 * CHD / LambdaNP2
8638  +249779. * CHB / LambdaNP2
8639  +18912.8 * CHW / LambdaNP2
8640  -109936. * CHWB / LambdaNP2
8641  -5170.73 * CDHB / LambdaNP2
8642  +3167.65 * CDHW / LambdaNP2
8643  +174267. * CuW_33r / LambdaNP2
8644  +3032981. * CuB_33r / LambdaNP2
8645  -0.388 * DeltaGF()
8646  +3.51 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8647  ;
8648 
8649  // Add modifications due to small variations of the SM parameters
8650  mu += cHSM * ( -1.319 * deltaMz()
8651  -9.866 * deltaMh()
8652  +2.617 * deltaaMZ()
8653  +0.421 * deltaGmu()
8654  -18.44 * deltamt() );
8655 
8656  } else if (Pol_em == -80. && Pol_ep == 30.){
8657  mu +=
8658  +121809. * CHbox / LambdaNP2
8659  +116253. * CHL1_11 / LambdaNP2
8660  +3415.4 * CHe_11 / LambdaNP2
8661  -98311.8 * CHu_11 / LambdaNP2
8662  +116253. * CHL3_11 / LambdaNP2
8663  -121117. * CuH_33r / LambdaNP2
8664  -81321.2 * CHD / LambdaNP2
8665  +87352.2 * CHB / LambdaNP2
8666  +182702. * CHW / LambdaNP2
8667  -319427. * CHWB / LambdaNP2
8668  -21.616 * CDHB / LambdaNP2
8669  +799.81 * CDHW / LambdaNP2
8670  +1948272. * CuW_33r / LambdaNP2
8671  +1078489. * CuB_33r / LambdaNP2
8672  -2.697 * DeltaGF()
8673  -3.37 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8674  ;
8675 
8676  // Add modifications due to small variations of the SM parameters
8677  mu += cHSM * ( +3.441 * deltaMz()
8678  -9.806 * deltaMh()
8679  +0.308 * deltaaMZ()
8680  +2.725 * deltaGmu()
8681  -18.491 * deltamt() );
8682 
8683  } else if (Pol_em == 80. && Pol_ep == 0.){
8684  mu +=
8685  +121837. * CHbox / LambdaNP2
8686  +24323.6 * CHL1_11 / LambdaNP2
8687  +111998. * CHe_11 / LambdaNP2
8688  +91391.1 * CHu_11 / LambdaNP2
8689  +24323.6 * CHL3_11 / LambdaNP2
8690  -123203. * CuH_33r / LambdaNP2
8691  -19404.2 * CHD / LambdaNP2
8692  +233452. * CHB / LambdaNP2
8693  +35310.2 * CHW / LambdaNP2
8694  -131019. * CHWB / LambdaNP2
8695  -4810.06 * CDHB / LambdaNP2
8696  +2842.31 * CDHW / LambdaNP2
8697  +351790. * CuW_33r / LambdaNP2
8698  +2837005. * CuB_33r / LambdaNP2
8699  -0.617 * DeltaGF()
8700  +2.818 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8701  ;
8702 
8703  // Add modifications due to small variations of the SM parameters
8704  mu += cHSM * ( -0.843 * deltaMz()
8705  -9.86 * deltaMh()
8706  +2.385 * deltaaMZ()
8707  +0.645 * deltaGmu()
8708  -18.45 * deltamt() );
8709 
8710  } else if (Pol_em == -80. && Pol_ep == 0.){
8711  mu +=
8712  +121814. * CHbox / LambdaNP2
8713  +113858. * CHL1_11 / LambdaNP2
8714  +6221.44 * CHe_11 / LambdaNP2
8715  -93321.6 * CHu_11 / LambdaNP2
8716  +113858. * CHL3_11 / LambdaNP2
8717  -121180. * CuH_33r / LambdaNP2
8718  -79695. * CHD / LambdaNP2
8719  +91201.9 * CHB / LambdaNP2
8720  +178853. * CHW / LambdaNP2
8721  -314513. * CHWB / LambdaNP2
8722  -137.642 * CDHB / LambdaNP2
8723  +853.383 * CDHW / LambdaNP2
8724  +1906734. * CuW_33r / LambdaNP2
8725  +1124181. * CuB_33r / LambdaNP2
8726  -2.642 * DeltaGF()
8727  -3.21 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8728  ;
8729 
8730  // Add modifications due to small variations of the SM parameters
8731  mu += cHSM * ( +3.33 * deltaMz()
8732  -9.807 * deltaMh()
8733  +0.362 * deltaaMZ()
8734  +2.671 * deltaGmu()
8735  -18.489 * deltamt() );
8736 
8737  } else {
8738  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
8739  }
8740 
8741  } else if (sqrt_s == 1.0) {
8742 
8743  C1 = 0.017;
8744 
8745  if (Pol_em == 80. && Pol_ep == -30.){
8746  mu +=
8747  +122269. * CHbox / LambdaNP2
8748  +148925. * CHL1_11 / LambdaNP2
8749  -1516295. * CHe_11 / LambdaNP2
8750  +181376. * CHu_11 / LambdaNP2
8751  +148925. * CHL3_11 / LambdaNP2
8752  -115721. * CuH_33r / LambdaNP2
8753  -9966.97 * CHD / LambdaNP2
8754  +648027. * CHB / LambdaNP2
8755  +58990.6 * CHW / LambdaNP2
8756  -166947. * CHWB / LambdaNP2
8757  +258446. * CDHB / LambdaNP2
8758  +27641. * CDHW / LambdaNP2
8759  +416063. * CuW_33r / LambdaNP2
8760  +5771745. * CuB_33r / LambdaNP2
8761  -0.426 * DeltaGF()
8762  +3.026 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8763  ;
8764 
8765  // Add modifications due to small variations of the SM parameters
8766  mu += cHSM * ( -1.159 * deltaMz()
8767  -1.211 * deltaMh()
8768  +2.586 * deltaaMZ()
8769  +0.445 * deltaGmu()
8770  +2.101 * deltamt() );
8771 
8772  } else if (Pol_em == -80. && Pol_ep == 30.){
8773  mu +=
8774  +122212. * CHbox / LambdaNP2
8775  +1266376. * CHL1_11 / LambdaNP2
8776  -47326.8 * CHe_11 / LambdaNP2
8777  -104685. * CHu_11 / LambdaNP2
8778  +1266376. * CHL3_11 / LambdaNP2
8779  -116193. * CuH_33r / LambdaNP2
8780  -85861. * CHD / LambdaNP2
8781  +202732. * CHB / LambdaNP2
8782  +516612. * CHW / LambdaNP2
8783  -514723. * CHWB / LambdaNP2
8784  -75504.5 * CDHB / LambdaNP2
8785  +158356. * CDHW / LambdaNP2
8786  +3954267. * CuW_33r / LambdaNP2
8787  +2288387. * CuB_33r / LambdaNP2
8788  -2.929 * DeltaGF()
8789  -5.432 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8790  ;
8791 
8792  // Add modifications due to small variations of the SM parameters
8793  mu += cHSM * ( +3.902 * deltaMz()
8794  -1.192 * deltaMh()
8795  +0.075 * deltaaMZ()
8796  +2.94 * deltaGmu()
8797  +2.16 * deltamt() );
8798 
8799  } else if (Pol_em == 80. && Pol_ep == 0.){
8800  mu +=
8801  +122564. * CHbox / LambdaNP2
8802  +252265. * CHL1_11 / LambdaNP2
8803  -1381101. * CHe_11 / LambdaNP2
8804  +155161. * CHu_11 / LambdaNP2
8805  +252265. * CHL3_11 / LambdaNP2
8806  -115358. * CuH_33r / LambdaNP2
8807  -16813.1 * CHD / LambdaNP2
8808  +607466. * CHB / LambdaNP2
8809  +101359. * CHW / LambdaNP2
8810  -198737. * CHWB / LambdaNP2
8811  +227834. * CDHB / LambdaNP2
8812  +39939.6 * CDHW / LambdaNP2
8813  +742520. * CuW_33r / LambdaNP2
8814  +5453267. * CuB_33r / LambdaNP2
8815  -0.659 * DeltaGF()
8816  +2.273 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8817  ;
8818 
8819  // Add modifications due to small variations of the SM parameters
8820  mu += cHSM * ( -0.69 * deltaMz()
8821  -1.205 * deltaMh()
8822  +2.349 * deltaaMZ()
8823  +0.676 * deltaGmu()
8824  +2.105 * deltamt() );
8825 
8826  } else if (Pol_em == -80. && Pol_ep == 0.){
8827  mu +=
8828  +122380. * CHbox / LambdaNP2
8829  +1238124. * CHL1_11 / LambdaNP2
8830  -84811.2 * CHe_11 / LambdaNP2
8831  -97259.2 * CHu_11 / LambdaNP2
8832  +1238124. * CHL3_11 / LambdaNP2
8833  -116044. * CuH_33r / LambdaNP2
8834  -83798.9 * CHD / LambdaNP2
8835  +214128. * CHB / LambdaNP2
8836  +505118. * CHW / LambdaNP2
8837  -505830. * CHWB / LambdaNP2
8838  -66814.1 * CDHB / LambdaNP2
8839  +155075. * CDHW / LambdaNP2
8840  +3863710. * CuW_33r / LambdaNP2
8841  +2378351. * CuB_33r / LambdaNP2
8842  -2.867 * DeltaGF()
8843  -5.212 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8844  ;
8845 
8846  // Add modifications due to small variations of the SM parameters
8847  mu += cHSM * ( +3.771 * deltaMz()
8848  -1.195 * deltaMh()
8849  +0.137 * deltaaMZ()
8850  +2.878 * deltaGmu()
8851  +2.166 * deltamt() );
8852 
8853  } else {
8854  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
8855  }
8856 
8857  } else if (sqrt_s == 1.4) {
8858 
8859  C1 = 0.0094;
8860 
8861  if (Pol_em == 80. && Pol_ep == -30.){
8862  mu +=
8863  +121945. * CHbox / LambdaNP2
8864  +416437. * CHL1_11 / LambdaNP2
8865  -5198451. * CHe_11 / LambdaNP2
8866  +211446. * CHu_11 / LambdaNP2
8867  +416437. * CHL3_11 / LambdaNP2
8868  -110413. * CuH_33r / LambdaNP2
8869  -8089.5 * CHD / LambdaNP2
8870  +852065. * CHB / LambdaNP2
8871  +78915.7 * CHW / LambdaNP2
8872  -191411. * CHWB / LambdaNP2
8873  +881670. * CDHB / LambdaNP2
8874  +72289.2 * CDHW / LambdaNP2
8875  +588296. * CuW_33r / LambdaNP2
8876  +7812392. * CuB_33r / LambdaNP2
8877  -0.441 * DeltaGF()
8878  +2.819 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8879  ;
8880 
8881  // Add modifications due to small variations of the SM parameters
8882  mu += cHSM * ( -1.109 * deltaMz()
8883  -0.905 * deltaMh()
8884  +2.571 * deltaaMZ()
8885  +0.451 * deltaGmu()
8886  +2.225 * deltamt() );
8887 
8888  } else if (Pol_em == -80. && Pol_ep == 30.){
8889  mu +=
8890  +122124. * CHbox / LambdaNP2
8891  +3668482. * CHL1_11 / LambdaNP2
8892  -164738. * CHe_11 / LambdaNP2
8893  -106285. * CHu_11 / LambdaNP2
8894  +3668482. * CHL3_11 / LambdaNP2
8895  -112775. * CuH_33r / LambdaNP2
8896  -87497.2 * CHD / LambdaNP2
8897  +261266. * CHB / LambdaNP2
8898  +703789. * CHW / LambdaNP2
8899  -618584. * CHWB / LambdaNP2
8900  -257636. * CDHB / LambdaNP2
8901  +530202. * CDHW / LambdaNP2
8902  +5501929. * CuW_33r / LambdaNP2
8903  +3213842. * CuB_33r / LambdaNP2
8904  -3.038 * DeltaGF()
8905  -6.378 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8906  ;
8907 
8908  // Add modifications due to small variations of the SM parameters
8909  mu += cHSM * ( +4.12 * deltaMz()
8910  -0.898 * deltaMh()
8911  -0.029 * deltaaMZ()
8912  +3.056 * deltaGmu()
8913  +2.28 * deltamt() );
8914 
8915  } else if (Pol_em == 80. && Pol_ep == 0.){
8916  mu +=
8917  +121843. * CHbox / LambdaNP2
8918  +706068. * CHL1_11 / LambdaNP2
8919  -4748505. * CHe_11 / LambdaNP2
8920  +182964. * CHu_11 / LambdaNP2
8921  +706068. * CHL3_11 / LambdaNP2
8922  -110672. * CuH_33r / LambdaNP2
8923  -15249.5 * CHD / LambdaNP2
8924  +798771. * CHB / LambdaNP2
8925  +134415. * CHW / LambdaNP2
8926  -229663. * CHWB / LambdaNP2
8927  +779863. * CDHB / LambdaNP2
8928  +112951. * CDHW / LambdaNP2
8929  +1026697. * CuW_33r / LambdaNP2
8930  +7402171. * CuB_33r / LambdaNP2
8931  -0.673 * DeltaGF()
8932  +1.996 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8933  ;
8934 
8935  // Add modifications due to small variations of the SM parameters
8936  mu += cHSM * ( -0.648 * deltaMz()
8937  -0.901 * deltaMh()
8938  +2.34 * deltaaMZ()
8939  +0.693 * deltaGmu()
8940  +2.232 * deltamt() );
8941 
8942  } else if (Pol_em == -80. && Pol_ep == 0.){
8943  mu +=
8944  +122069. * CHbox / LambdaNP2
8945  +3581543. * CHL1_11 / LambdaNP2
8946  -298692. * CHe_11 / LambdaNP2
8947  -97874.3 * CHu_11 / LambdaNP2
8948  +3581543. * CHL3_11 / LambdaNP2
8949  -112737. * CuH_33r / LambdaNP2
8950  -85431.2 * CHD / LambdaNP2
8951  +276629. * CHB / LambdaNP2
8952  +687136. * CHW / LambdaNP2
8953  -607155. * CHWB / LambdaNP2
8954  -227375. * CDHB / LambdaNP2
8955  +517945. * CDHW / LambdaNP2
8956  +5370183. * CuW_33r / LambdaNP2
8957  +3335906. * CuB_33r / LambdaNP2
8958  -2.969 * DeltaGF()
8959  -6.138 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8960  ;
8961 
8962  // Add modifications due to small variations of the SM parameters
8963  mu += cHSM * ( +3.976 * deltaMz()
8964  -0.895 * deltaMh()
8965  +0.039 * deltaaMZ()
8966  +2.986 * deltaGmu()
8967  +2.271 * deltamt() );
8968 
8969  } else {
8970  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
8971  }
8972 
8973  } else if (sqrt_s == 1.5) {
8974 
8975  C1 = 0.0094;// Use the same as 1400 GeV
8976 
8977  if (Pol_em == 80. && Pol_ep == -30.){
8978  mu +=
8979  +121854. * CHbox / LambdaNP2
8980  +507190. * CHL1_11 / LambdaNP2
8981  -6475118. * CHe_11 / LambdaNP2
8982  +216935. * CHu_11 / LambdaNP2
8983  +507190. * CHL3_11 / LambdaNP2
8984  -109820. * CuH_33r / LambdaNP2
8985  -7568.59 * CHD / LambdaNP2
8986  +893094. * CHB / LambdaNP2
8987  +82781.5 * CHW / LambdaNP2
8988  -196556. * CHWB / LambdaNP2
8989  +1099527. * CDHB / LambdaNP2
8990  +87228. * CDHW / LambdaNP2
8991  +630747. * CuW_33r / LambdaNP2
8992  +8328477. * CuB_33r / LambdaNP2
8993  -0.442 * DeltaGF()
8994  +2.756 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
8995  ;
8996 
8997  // Add modifications due to small variations of the SM parameters
8998  mu += cHSM * ( -1.104 * deltaMz()
8999  -0.856 * deltaMh()
9000  +2.568 * deltaaMZ()
9001  +0.455 * deltaGmu()
9002  +2.232 * deltamt() );
9003 
9004  } else if (Pol_em == -80. && Pol_ep == 30.){
9005  mu +=
9006  +121994. * CHbox / LambdaNP2
9007  +4501280. * CHL1_11 / LambdaNP2
9008  -206085. * CHe_11 / LambdaNP2
9009  -106381. * CHu_11 / LambdaNP2
9010  +4501280. * CHL3_11 / LambdaNP2
9011  -112104. * CuH_33r / LambdaNP2
9012  -87805.6 * CHD / LambdaNP2
9013  +273106. * CHB / LambdaNP2
9014  +741955. * CHW / LambdaNP2
9015  -639545. * CHWB / LambdaNP2
9016  -322155. * CDHB / LambdaNP2
9017  +661931. * CDHW / LambdaNP2
9018  +5892414. * CuW_33r / LambdaNP2
9019  +3448015. * CuB_33r / LambdaNP2
9020  -3.057 * DeltaGF()
9021  -6.552 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9022  ;
9023 
9024  // Add modifications due to small variations of the SM parameters
9025  mu += cHSM * ( +4.154 * deltaMz()
9026  -0.856 * deltaMh()
9027  -0.045 * deltaaMZ()
9028  +3.071 * deltaGmu()
9029  +2.287 * deltamt() );
9030 
9031  } else if (Pol_em == 80. && Pol_ep == 0.){
9032  mu +=
9033  +121793. * CHbox / LambdaNP2
9034  +861242. * CHL1_11 / LambdaNP2
9035  -5919951. * CHe_11 / LambdaNP2
9036  +188249. * CHu_11 / LambdaNP2
9037  +861242. * CHL3_11 / LambdaNP2
9038  -109696. * CuH_33r / LambdaNP2
9039  -14806.7 * CHD / LambdaNP2
9040  +837632. * CHB / LambdaNP2
9041  +141142. * CHW / LambdaNP2
9042  -235907. * CHWB / LambdaNP2
9043  +973107. * CDHB / LambdaNP2
9044  +138331. * CDHW / LambdaNP2
9045  +1097452. * CuW_33r / LambdaNP2
9046  +7895510. * CuB_33r / LambdaNP2
9047  -0.673 * DeltaGF()
9048  +1.935 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9049  ;
9050 
9051  // Add modifications due to small variations of the SM parameters
9052  mu += cHSM * ( -0.637 * deltaMz()
9053  -0.859 * deltaMh()
9054  +2.339 * deltaaMZ()
9055  +0.68 * deltaGmu()
9056  +2.236 * deltamt() );
9057 
9058  } else if (Pol_em == -80. && Pol_ep == 0.){
9059  mu +=
9060  +122029. * CHbox / LambdaNP2
9061  +4394189. * CHL1_11 / LambdaNP2
9062  -373205. * CHe_11 / LambdaNP2
9063  -97750.6 * CHu_11 / LambdaNP2
9064  +4394189. * CHL3_11 / LambdaNP2
9065  -112024. * CuH_33r / LambdaNP2
9066  -85643.3 * CHD / LambdaNP2
9067  +289620. * CHB / LambdaNP2
9068  +724463. * CHW / LambdaNP2
9069  -627885. * CHWB / LambdaNP2
9070  -284076. * CDHB / LambdaNP2
9071  +646658. * CDHW / LambdaNP2
9072  +5753330. * CuW_33r / LambdaNP2
9073  +3578793. * CuB_33r / LambdaNP2
9074  -2.989 * DeltaGF()
9075  -6.311 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9076  ;
9077 
9078  // Add modifications due to small variations of the SM parameters
9079  mu += cHSM * ( +4.014 * deltaMz()
9080  -0.855 * deltaMh()
9081  +0.024 * deltaaMZ()
9082  +3.011 * deltaGmu()
9083  +2.286 * deltamt() );
9084 
9085  } else {
9086  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9087  }
9088 
9089  } else if (sqrt_s == 3.0) {
9090 
9091  C1 = 0.0037;
9092 
9093  if (Pol_em == 80. && Pol_ep == -30.){
9094  mu +=
9095  +122442. * CHbox / LambdaNP2
9096  +3092340. * CHL1_11 / LambdaNP2
9097  -43264264. * CHe_11 / LambdaNP2
9098  +259622. * CHu_11 / LambdaNP2
9099  +3092340. * CHL3_11 / LambdaNP2
9100  -100510. * CuH_33r / LambdaNP2
9101  -3230.01 * CHD / LambdaNP2
9102  +1267548. * CHB / LambdaNP2
9103  +118886. * CHW / LambdaNP2
9104  -247164. * CHWB / LambdaNP2
9105  +7397753. * CDHB / LambdaNP2
9106  +510206. * CDHW / LambdaNP2
9107  +1343630. * CuW_33r / LambdaNP2
9108  +17234081. * CuB_33r / LambdaNP2
9109  -0.459 * DeltaGF()
9110  +2.453 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9111  ;
9112 
9113  // Add modifications due to small variations of the SM parameters
9114  mu += cHSM * ( -1.07 * deltaMz()
9115  -0.576 * deltaMh()
9116  +2.542 * deltaaMZ()
9117  +0.468 * deltaGmu()
9118  +2.145 * deltamt() );
9119 
9120  } else if (Pol_em == -80. && Pol_ep == 30.){
9121  mu +=
9122  +122230. * CHbox / LambdaNP2
9123  +28686134. * CHL1_11 / LambdaNP2
9124  -1435177. * CHe_11 / LambdaNP2
9125  -108195. * CHu_11 / LambdaNP2
9126  +28686134. * CHL3_11 / LambdaNP2
9127  -105858. * CuH_33r / LambdaNP2
9128  -89803.1 * CHD / LambdaNP2
9129  +381886. * CHB / LambdaNP2
9130  +1102843. * CHW / LambdaNP2
9131  -834821. * CHWB / LambdaNP2
9132  -2237555. * CDHB / LambdaNP2
9133  +4557030. * CDHW / LambdaNP2
9134  +12639913. * CuW_33r / LambdaNP2
9135  +7455995. * CuB_33r / LambdaNP2
9136  -3.212 * DeltaGF()
9137  -8.009 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9138  ;
9139 
9140  // Add modifications due to small variations of the SM parameters
9141  mu += cHSM * ( +4.469 * deltaMz()
9142  -0.595 * deltaMh()
9143  -0.222 * deltaaMZ()
9144  +3.22 * deltaGmu()
9145  +2.195 * deltamt() );
9146 
9147  } else if (Pol_em == 80. && Pol_ep == 0.){
9148  mu +=
9149  +122688. * CHbox / LambdaNP2
9150  +5271741. * CHL1_11 / LambdaNP2
9151  -39707692. * CHe_11 / LambdaNP2
9152  +228729. * CHu_11 / LambdaNP2
9153  +5271741. * CHL3_11 / LambdaNP2
9154  -100891. * CuH_33r / LambdaNP2
9155  -10526.3 * CHD / LambdaNP2
9156  +1192421. * CHB / LambdaNP2
9157  +202915. * CHW / LambdaNP2
9158  -296939. * CHWB / LambdaNP2
9159  +6582510. * CDHB / LambdaNP2
9160  +853895. * CDHW / LambdaNP2
9161  +2303644. * CuW_33r / LambdaNP2
9162  +16407287. * CuB_33r / LambdaNP2
9163  -0.693 * DeltaGF()
9164  +1.565 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9165  ;
9166 
9167  // Add modifications due to small variations of the SM parameters
9168  mu += cHSM * ( -0.597 * deltaMz()
9169  -0.565 * deltaMh()
9170  +2.305 * deltaaMZ()
9171  +0.708 * deltaGmu()
9172  +2.153 * deltamt() );
9173 
9174  } else if (Pol_em == -80. && Pol_ep == 0.){
9175  mu +=
9176  +121781. * CHbox / LambdaNP2
9177  +27966374. * CHL1_11 / LambdaNP2
9178  -2597153. * CHe_11 / LambdaNP2
9179  -98089.4 * CHu_11 / LambdaNP2
9180  +27966374. * CHL3_11 / LambdaNP2
9181  -105885. * CuH_33r / LambdaNP2
9182  -87600.3 * CHD / LambdaNP2
9183  +406305. * CHB / LambdaNP2
9184  +1075086. * CHW / LambdaNP2
9185  -818808. * CHWB / LambdaNP2
9186  -1967062. * CDHB / LambdaNP2
9187  +4442109. * CDHW / LambdaNP2
9188  +12322125. * CuW_33r / LambdaNP2
9189  +7728315. * CuB_33r / LambdaNP2
9190  -3.134 * DeltaGF()
9191  -7.724 * 0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
9192  ;
9193 
9194  // Add modifications due to small variations of the SM parameters
9195  mu += cHSM * ( +4.305 * deltaMz()
9196  -0.59 * deltaMh()
9197  -0.147 * deltaaMZ()
9198  +3.144 * deltaGmu()
9199  +2.192 * deltamt() );
9200 
9201  } else {
9202  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9203  }
9204 
9205  } else
9206  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9207 
9208  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9209  mu += eeettHint + eeettHpar;
9210 
9211 // Linear contribution from Higgs self-coupling
9212  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9213 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9215 
9216  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9217 
9218  return mu;
9219 }
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3650
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3651
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2410
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ mueeWBF()

double NPSMEFTd6::mueeWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 3452 of file NPSMEFTd6.cpp.

3453 {
3454  double mu = 1.0;
3455 
3456  double C1 = 0.0;
3457 
3458  if (sqrt_s == 0.240) {
3459 
3460  C1 = 0.0064;
3461 
3462  mu +=
3463  +121120. * CHbox / LambdaNP2
3464  -138682. * CHL3_11 / LambdaNP2
3465  -203727. * CHD / LambdaNP2
3466  -24699.7 * CHW / LambdaNP2
3467  -379830. * CHWB / LambdaNP2
3468  -18173.7 * CDHW / LambdaNP2
3469  -4.716 * DeltaGF()
3470  -5.665 * deltaMwd6()
3471  ;
3472 
3473  // Add modifications due to small variations of the SM parameters
3474  mu += cHSM * (
3475  +3.307 * deltaMz()
3476  -3.995 * deltaMh()
3477  -0.486 * deltaaMZ()
3478  +3.507 * deltaGmu() );
3479 
3480  if (FlagQuadraticTerms) {
3481  //Add contributions that are quadratic in the effective coefficients
3482  mu += 0.0;
3483  }
3484 
3485  } else if (sqrt_s == 0.250) {
3486 
3487  C1 = 0.0064;
3488 
3489  mu +=
3490  +121142. * CHbox / LambdaNP2
3491  -147357. * CHL3_11 / LambdaNP2
3492  -203726. * CHD / LambdaNP2
3493  -26559.2 * CHW / LambdaNP2
3494  -379797. * CHWB / LambdaNP2
3495  -19265.3 * CDHW / LambdaNP2
3496  -4.717 * DeltaGF()
3497  -5.593 * deltaMwd6()
3498  ;
3499 
3500  // Add modifications due to small variations of the SM parameters
3501  mu += cHSM * (
3502  +3.413 * deltaMz()
3503  -3.644 * deltaMh()
3504  -0.502 * deltaaMZ()
3505  +3.523 * deltaGmu() );
3506 
3507  if (FlagQuadraticTerms) {
3508  //Add contributions that are quadratic in the effective coefficients
3509  mu += 0.0;
3510  }
3511 
3512  } else if (sqrt_s == 0.350) {
3513 
3514  C1 = 0.0062;
3515 
3516  mu +=
3517  +121107. * CHbox / LambdaNP2
3518  -219582. * CHL3_11 / LambdaNP2
3519  -203717. * CHD / LambdaNP2
3520  -39722.3 * CHW / LambdaNP2
3521  -379795. * CHWB / LambdaNP2
3522  -28864.2 * CDHW / LambdaNP2
3523  -4.714 * DeltaGF()
3524  -5.13 * deltaMwd6()
3525  ;
3526 
3527  // Add modifications due to small variations of the SM parameters
3528  mu += cHSM * (
3529  +4.073 * deltaMz()
3530  -1.94 * deltaMh()
3531  -0.598 * deltaaMZ()
3532  +3.623 * deltaGmu() );
3533 
3534  if (FlagQuadraticTerms) {
3535  //Add contributions that are quadratic in the effective coefficients
3536  mu += 0.0;
3537  }
3538 
3539  } else if (sqrt_s == 0.365) {
3540 
3541  C1 = 0.0062; // Use the same as 350 GeV
3542 
3543  mu +=
3544  +121071. * CHbox / LambdaNP2
3545  -228452. * CHL3_11 / LambdaNP2
3546  -203725. * CHD / LambdaNP2
3547  -40966.9 * CHW / LambdaNP2
3548  -379798. * CHWB / LambdaNP2
3549  -30110.4 * CDHW / LambdaNP2
3550  -4.714 * DeltaGF()
3551  -5.08 * deltaMwd6()
3552  ;
3553 
3554  // Add modifications due to small variations of the SM parameters
3555  mu += cHSM * (
3556  +4.136 * deltaMz()
3557  -1.817 * deltaMh()
3558  -0.609 * deltaaMZ()
3559  +3.635 * deltaGmu() );
3560 
3561  if (FlagQuadraticTerms) {
3562  //Add contributions that are quadratic in the effective coefficients
3563  mu += 0.0;
3564  }
3565 
3566  } else if (sqrt_s == 0.380) {
3567 
3568  C1 = 0.0062; // Use the same as 350 GeV
3569 
3570  mu +=
3571  +121001. * CHbox / LambdaNP2
3572  -237126. * CHL3_11 / LambdaNP2
3573  -203726. * CHD / LambdaNP2
3574  -42070.9 * CHW / LambdaNP2
3575  -379788. * CHWB / LambdaNP2
3576  -31352.7 * CDHW / LambdaNP2
3577  -4.714 * DeltaGF()
3578  -5.044 * deltaMwd6()
3579  ;
3580 
3581  // Add modifications due to small variations of the SM parameters
3582  mu += cHSM * (
3583  +4.192 * deltaMz()
3584  -1.711 * deltaMh()
3585  -0.618 * deltaaMZ()
3586  +3.64 * deltaGmu() );
3587 
3588  if (FlagQuadraticTerms) {
3589  //Add contributions that are quadratic in the effective coefficients
3590  mu += 0.0;
3591  }
3592 
3593  } else if (sqrt_s == 0.500) {
3594 
3595  C1 = 0.0061;
3596 
3597  mu +=
3598  +121063. * CHbox / LambdaNP2
3599  -295115. * CHL3_11 / LambdaNP2
3600  -203679. * CHD / LambdaNP2
3601  -47539.5 * CHW / LambdaNP2
3602  -379773. * CHWB / LambdaNP2
3603  -39825.1 * CDHW / LambdaNP2
3604  -4.715 * DeltaGF()
3605  -4.817 * deltaMwd6()
3606  ;
3607 
3608  // Add modifications due to small variations of the SM parameters
3609  mu += cHSM * (
3610  +4.509 * deltaMz()
3611  -1.178 * deltaMh()
3612  -0.666 * deltaaMZ()
3613  +3.692 * deltaGmu() );
3614 
3615  if (FlagQuadraticTerms) {
3616  //Add contributions that are quadratic in the effective coefficients
3617  mu += 0.0;
3618  }
3619 
3620  } else if (sqrt_s == 1.0) {
3621 
3622  C1 = 0.0059;
3623 
3624  mu +=
3625  +120960. * CHbox / LambdaNP2
3626  -442647. * CHL3_11 / LambdaNP2
3627  -203748. * CHD / LambdaNP2
3628  -49375.4 * CHW / LambdaNP2
3629  -379685. * CHWB / LambdaNP2
3630  -63503.9 * CDHW / LambdaNP2
3631  -4.712 * DeltaGF()
3632  -4.481 * deltaMwd6()
3633  ;
3634 
3635  // Add modifications due to small variations of the SM parameters
3636  mu += cHSM * (
3637  +4.99 * deltaMz()
3638  -0.582 * deltaMh()
3639  -0.734 * deltaaMZ()
3640  +3.765 * deltaGmu() );
3641 
3642  if (FlagQuadraticTerms) {
3643  //Add contributions that are quadratic in the effective coefficients
3644  mu += 0.0;
3645  }
3646 
3647  } else if (sqrt_s == 1.4) {
3648 
3649  C1 = 0.0058;
3650 
3651  mu +=
3652  +121118. * CHbox / LambdaNP2
3653  -515189. * CHL3_11 / LambdaNP2
3654  -203684. * CHD / LambdaNP2
3655  -46619.5 * CHW / LambdaNP2
3656  -379667. * CHWB / LambdaNP2
3657  -75747.8 * CDHW / LambdaNP2
3658  -4.714 * DeltaGF()
3659  -4.391 * deltaMwd6()
3660  ;
3661 
3662  // Add modifications due to small variations of the SM parameters
3663  mu += cHSM * (
3664  +5.13 * deltaMz()
3665  -0.446 * deltaMh()
3666  -0.754 * deltaaMZ()
3667  +3.784 * deltaGmu() );
3668 
3669  if (FlagQuadraticTerms) {
3670  //Add contributions that are quadratic in the effective coefficients
3671  mu += 0.0;
3672  }
3673 
3674  } else if (sqrt_s == 1.5) {
3675 
3676  C1 = 0.0058;// Use the same as 1400 GeV
3677 
3678  mu +=
3679  +121200. * CHbox / LambdaNP2
3680  -530152. * CHL3_11 / LambdaNP2
3681  -203649. * CHD / LambdaNP2
3682  -45921.3 * CHW / LambdaNP2
3683  -379591. * CHWB / LambdaNP2
3684  -78241.3 * CDHW / LambdaNP2
3685  -4.715 * DeltaGF()
3686  -4.38 * deltaMwd6()
3687  ;
3688 
3689  // Add modifications due to small variations of the SM parameters
3690  mu += cHSM * (
3691  +5.154 * deltaMz()
3692  -0.424 * deltaMh()
3693  -0.757 * deltaaMZ()
3694  +3.786 * deltaGmu() );
3695 
3696  if (FlagQuadraticTerms) {
3697  //Add contributions that are quadratic in the effective coefficients
3698  mu += 0.0;
3699  }
3700 
3701  } else if (sqrt_s == 3.0) {
3702 
3703  C1 = 0.0057;
3704 
3705  mu +=
3706  +121321. * CHbox / LambdaNP2
3707  -684382. * CHL3_11 / LambdaNP2
3708  -203585. * CHD / LambdaNP2
3709  -38239. * CHW / LambdaNP2
3710  -379518. * CHWB / LambdaNP2
3711  -104465. * CDHW / LambdaNP2
3712  -4.714 * DeltaGF()
3713  -4.258 * deltaMwd6()
3714  ;
3715 
3716  // Add modifications due to small variations of the SM parameters
3717  mu += cHSM * (
3718  +5.331 * deltaMz()
3719  -0.279 * deltaMh()
3720  -0.785 * deltaaMZ()
3721  +3.81 * deltaGmu() );
3722 
3723  if (FlagQuadraticTerms) {
3724  //Add contributions that are quadratic in the effective coefficients
3725  mu += 0.0;
3726  }
3727 
3728  } else
3729  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWBF()");
3730 
3731  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3732  mu += eeeWBFint + eeeWBFpar;
3733 
3734 // Linear contribution from Higgs self-coupling
3735  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3736 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3738 
3739  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3740 
3741  return mu;
3742 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeWBFPol()

double NPSMEFTd6::mueeWBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 3745 of file NPSMEFTd6.cpp.

3746 {
3747 
3748 // Pure WBF, hence only initiated by LH fermions. No difference between polarizations at the linear level.
3749 // Expand like other functions when quadratic terms are included
3750 
3751  return mueeWBF(sqrt_s);
3752 }
virtual double mueeWBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model...
Definition: NPSMEFTd6.cpp:3452

◆ mueeZBF()

double NPSMEFTd6::mueeZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5073 of file NPSMEFTd6.cpp.

5074 {
5075  double mu = 1.0;
5076 
5077  double C1 = 0.0;
5078 
5079  if (sqrt_s == 0.240) {
5080 
5081  C1 = 0.0070;
5082 
5083  mu +=
5084  +121661. * CHbox / LambdaNP2
5085  +489617. * CHL1_11 / LambdaNP2
5086  -357163. * CHe_11 / LambdaNP2
5087  +489617. * CHL3_11 / LambdaNP2
5088  -39217.8 * CHD / LambdaNP2
5089  +1525468. * CHB / LambdaNP2
5090  +378019. * CHW / LambdaNP2
5091  +215983. * CHWB / LambdaNP2
5092  -6554.11 * CDHB / LambdaNP2
5093  +1175.47 * CDHW / LambdaNP2
5094  -3.161 * DeltaGF()
5095  ;
5096 
5097  // Add modifications due to small variations of the SM parameters
5098  mu += cHSM * ( +0.908 * deltaMz()
5099  -5.799 * deltaMh()
5100  -0.248 * deltaaMZ()
5101  +3.158 * deltaGmu() );
5102 
5103  if (FlagQuadraticTerms) {
5104  //Add contributions that are quadratic in the effective coefficients
5105  mu += 0.0;
5106  }
5107 
5108  } else if (sqrt_s == 0.250) {
5109 
5110  C1 = 0.0070;
5111 
5112  mu +=
5113  +122144. * CHbox / LambdaNP2
5114  +444406. * CHL1_11 / LambdaNP2
5115  -315727. * CHe_11 / LambdaNP2
5116  +444406. * CHL3_11 / LambdaNP2
5117  -41440.8 * CHD / LambdaNP2
5118  +1186855. * CHB / LambdaNP2
5119  +301913. * CHW / LambdaNP2
5120  +98540.5 * CHWB / LambdaNP2
5121  -5766.35 * CDHB / LambdaNP2
5122  +294.724 * CDHW / LambdaNP2
5123  -3.279 * DeltaGF()
5124  ;
5125 
5126  // Add modifications due to small variations of the SM parameters
5127  mu += cHSM * ( +2.044 * deltaMz()
5128  -4.578 * deltaMh()
5129  -0.341 * deltaaMZ()
5130  +3.283 * deltaGmu() );
5131 
5132  if (FlagQuadraticTerms) {
5133  //Add contributions that are quadratic in the effective coefficients
5134  mu += 0.0;
5135  }
5136 
5137  } else if (sqrt_s == 0.350) {
5138 
5139  C1 = 0.0069;
5140 
5141  mu +=
5142  +121556. * CHbox / LambdaNP2
5143  +46354.9 * CHL1_11 / LambdaNP2
5144  -251.929 * CHe_11 / LambdaNP2
5145  +46354.9 * CHL3_11 / LambdaNP2
5146  -43426.2 * CHD / LambdaNP2
5147  +450512. * CHB / LambdaNP2
5148  +166493. * CHW / LambdaNP2
5149  -198898. * CHWB / LambdaNP2
5150  -4408.76 * CDHB / LambdaNP2
5151  -17005.2 * CDHW / LambdaNP2
5152  -3.427 * DeltaGF()
5153  ;
5154 
5155  // Add modifications due to small variations of the SM parameters
5156  mu += cHSM * ( +3.845 * deltaMz()
5157  -1.857 * deltaMh()
5158  -0.423 * deltaaMZ()
5159  +3.407 * deltaGmu() );
5160 
5161  if (FlagQuadraticTerms) {
5162  //Add contributions that are quadratic in the effective coefficients
5163  mu += 0.0;
5164  }
5165 
5166  } else if (sqrt_s == 0.365) {
5167 
5168  C1 = 0.0069; // use same as 350 GeV
5169 
5170  mu +=
5171  +121067. * CHbox / LambdaNP2
5172  +9887.64 * CHL1_11 / LambdaNP2
5173  +27809. * CHe_11 / LambdaNP2
5174  +9887.64 * CHL3_11 / LambdaNP2
5175  -43174.2 * CHD / LambdaNP2
5176  +417865. * CHB / LambdaNP2
5177  +154270. * CHW / LambdaNP2
5178  -201517. * CHWB / LambdaNP2
5179  -4943.82 * CDHB / LambdaNP2
5180  -19213.5 * CDHW / LambdaNP2
5181  -3.423 * DeltaGF()
5182  ;
5183 
5184  // Add modifications due to small variations of the SM parameters
5185  mu += cHSM * ( +3.861 * deltaMz()
5186  -1.736 * deltaMh()
5187  -0.426 * deltaaMZ()
5188  +3.375 * deltaGmu() );
5189 
5190  if (FlagQuadraticTerms) {
5191  //Add contributions that are quadratic in the effective coefficients
5192  mu += 0.0;
5193  }
5194 
5195  } else if (sqrt_s == 0.380) {
5196 
5197  C1 = 0.0069; // use same as 350 GeV
5198 
5199  mu +=
5200  +121214. * CHbox / LambdaNP2
5201  -22289.7 * CHL1_11 / LambdaNP2
5202  +52903.2 * CHe_11 / LambdaNP2
5203  -22289.7 * CHL3_11 / LambdaNP2
5204  -43137.3 * CHD / LambdaNP2
5205  +388336. * CHB / LambdaNP2
5206  +140923. * CHW / LambdaNP2
5207  -202884. * CHWB / LambdaNP2
5208  -5363.69 * CDHB / LambdaNP2
5209  -21404.2 * CDHW / LambdaNP2
5210  -3.418 * DeltaGF()
5211  ;
5212 
5213  // Add modifications due to small variations of the SM parameters
5214  mu += cHSM * ( +3.887 * deltaMz()
5215  -1.633 * deltaMh()
5216  -0.419 * deltaaMZ()
5217  +3.393 * deltaGmu() );
5218 
5219  if (FlagQuadraticTerms) {
5220  //Add contributions that are quadratic in the effective coefficients
5221  mu += 0.0;
5222  }
5223 
5224  } else if (sqrt_s == 0.500) {
5225 
5226  C1 = 0.0067;
5227 
5228  mu +=
5229  +121453. * CHbox / LambdaNP2
5230  -185326. * CHL1_11 / LambdaNP2
5231  +178925. * CHe_11 / LambdaNP2
5232  -185326. * CHL3_11 / LambdaNP2
5233  -42051.6 * CHD / LambdaNP2
5234  +236945. * CHB / LambdaNP2
5235  +67833.5 * CHW / LambdaNP2
5236  -178623. * CHWB / LambdaNP2
5237  -8004.61 * CDHB / LambdaNP2
5238  -33567.3 * CDHW / LambdaNP2
5239  -3.416 * DeltaGF()
5240  ;
5241 
5242  // Add modifications due to small variations of the SM parameters
5243  mu += cHSM * ( +3.963 * deltaMz()
5244  -1.143 * deltaMh()
5245  -0.408 * deltaaMZ()
5246  +3.383 * deltaGmu() );
5247 
5248  if (FlagQuadraticTerms) {
5249  //Add contributions that are quadratic in the effective coefficients
5250  mu += 0.0;
5251  }
5252 
5253  } else if (sqrt_s == 1.0) {
5254 
5255  C1 = 0.0065;
5256 
5257  mu +=
5258  +121062. * CHbox / LambdaNP2
5259  -409543. * CHL1_11 / LambdaNP2
5260  +356730. * CHe_11 / LambdaNP2
5261  -409543. * CHL3_11 / LambdaNP2
5262  -42133.9 * CHD / LambdaNP2
5263  +69851. * CHB / LambdaNP2
5264  -14416.8 * CHW / LambdaNP2
5265  -113198. * CHWB / LambdaNP2
5266  -18688.4 * CDHB / LambdaNP2
5267  -61696. * CDHW / LambdaNP2
5268  -3.405 * DeltaGF()
5269  ;
5270 
5271  // Add modifications due to small variations of the SM parameters
5272  mu += cHSM * ( +4.216 * deltaMz()
5273  -0.546 * deltaMh()
5274  -0.407 * deltaaMZ()
5275  +3.393 * deltaGmu() );
5276 
5277  if (FlagQuadraticTerms) {
5278  //Add contributions that are quadratic in the effective coefficients
5279  mu += 0.0;
5280  }
5281 
5282  } else if (sqrt_s == 1.4) {
5283 
5284  C1 = 0.0065;
5285 
5286  mu +=
5287  +120749. * CHbox / LambdaNP2
5288  -493617. * CHL1_11 / LambdaNP2
5289  +426669. * CHe_11 / LambdaNP2
5290  -493617. * CHL3_11 / LambdaNP2
5291  -42486.9 * CHD / LambdaNP2
5292  +34633.1 * CHB / LambdaNP2
5293  -27609.6 * CHW / LambdaNP2
5294  -97014.2 * CHWB / LambdaNP2
5295  -23942.2 * CDHB / LambdaNP2
5296  -74940.3 * CDHW / LambdaNP2
5297  -3.405 * DeltaGF()
5298  ;
5299 
5300  // Add modifications due to small variations of the SM parameters
5301  mu += cHSM * ( +4.309 * deltaMz()
5302  -0.422 * deltaMh()
5303  -0.402 * deltaaMZ()
5304  +3.379 * deltaGmu() );
5305 
5306  if (FlagQuadraticTerms) {
5307  //Add contributions that are quadratic in the effective coefficients
5308  mu += 0.0;
5309  }
5310 
5311  } else if (sqrt_s == 1.5) {
5312 
5313  C1 = 0.0065;// Use the same as 1400 GeV
5314 
5315  mu +=
5316  +120587. * CHbox / LambdaNP2
5317  -510290. * CHL1_11 / LambdaNP2
5318  +440504. * CHe_11 / LambdaNP2
5319  -510290. * CHL3_11 / LambdaNP2
5320  -42529.6 * CHD / LambdaNP2
5321  +30448.1 * CHB / LambdaNP2
5322  -30741.2 * CHW / LambdaNP2
5323  -95903.3 * CHWB / LambdaNP2
5324  -25074.9 * CDHB / LambdaNP2
5325  -77634.5 * CDHW / LambdaNP2
5326  -3.401 * DeltaGF()
5327  ;
5328 
5329  // Add modifications due to small variations of the SM parameters
5330  mu += cHSM * ( +4.326 * deltaMz()
5331  -0.4 * deltaMh()
5332  -0.403 * deltaaMZ()
5333  +3.37 * deltaGmu() );
5334 
5335  if (FlagQuadraticTerms) {
5336  //Add contributions that are quadratic in the effective coefficients
5337  mu += 0.0;
5338  }
5339 
5340  } else if (sqrt_s == 3.0) {
5341 
5342  C1 = 0.0063;
5343 
5344  mu +=
5345  +120474. * CHbox / LambdaNP2
5346  -677185. * CHL1_11 / LambdaNP2
5347  +582037. * CHe_11 / LambdaNP2
5348  -677185. * CHL3_11 / LambdaNP2
5349  -42541.3 * CHD / LambdaNP2
5350  +6810.6 * CHB / LambdaNP2
5351  -32994.5 * CHW / LambdaNP2
5352  -78012.3 * CHWB / LambdaNP2
5353  -36250. * CDHB / LambdaNP2
5354  -105734. * CDHW / LambdaNP2
5355  -3.405 * DeltaGF()
5356  ;
5357 
5358  // Add modifications due to small variations of the SM parameters
5359  mu += cHSM * ( +4.463 * deltaMz()
5360  -0.265 * deltaMh()
5361  -0.405 * deltaaMZ()
5362  +3.351 * deltaGmu() );
5363 
5364  if (FlagQuadraticTerms) {
5365  //Add contributions that are quadratic in the effective coefficients
5366  mu += 0.0;
5367  }
5368 
5369  } else
5370  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBF()");
5371 
5372  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5373  //(Assume similar to WBF.)
5374  mu += eeeWBFint + eeeWBFpar;
5375 
5376 // Linear contribution from Higgs self-coupling
5377  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5378 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5380 
5381  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5382 
5383  return mu;
5384 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeZBFPol()

double NPSMEFTd6::mueeZBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5387 of file NPSMEFTd6.cpp.

5388 {
5389  double mu = 1.0;
5390 
5391  double C1 = 0.0;
5392 
5393  if (sqrt_s == 0.240) {
5394 
5395  C1 = 0.0070;
5396 
5397  if (Pol_em == 80. && Pol_ep == -30.){
5398  mu +=
5399  +121531. * CHbox / LambdaNP2
5400  +58943.5 * CHL1_11 / LambdaNP2
5401  -939512. * CHe_11 / LambdaNP2
5402  +58943.5 * CHL3_11 / LambdaNP2
5403  +77442.6 * CHD / LambdaNP2
5404  +2082256. * CHB / LambdaNP2
5405  +108043. * CHW / LambdaNP2
5406  +1362693. * CHWB / LambdaNP2
5407  +40385. * CDHB / LambdaNP2
5408  -21886. * CDHW / LambdaNP2
5409  +0.563 * DeltaGF()
5410  ;
5411 
5412  // Add modifications due to small variations of the SM parameters
5413  mu += cHSM * ( -6.582 * deltaMz()
5414  -5.732 * deltaMh()
5415  +3.573 * deltaaMZ()
5416  -0.708 * deltaGmu() );
5417 
5418  } else if (Pol_em == -80. && Pol_ep == 30.){
5419  mu +=
5420  +122065. * CHbox / LambdaNP2
5421  +905327. * CHL1_11 / LambdaNP2
5422  -55689. * CHe_11 / LambdaNP2
5423  +905327. * CHL3_11 / LambdaNP2
5424  -124548. * CHD / LambdaNP2
5425  +905057. * CHB / LambdaNP2
5426  +540185. * CHW / LambdaNP2
5427  -329708. * CHWB / LambdaNP2
5428  -37296.9 * CDHB / LambdaNP2
5429  +20497.1 * CDHW / LambdaNP2
5430  -5.854 * DeltaGF()
5431  ;
5432 
5433  // Add modifications due to small variations of the SM parameters
5434  mu += cHSM * ( +6.473 * deltaMz()
5435  -5.971 * deltaMh()
5436  -3.019 * deltaaMZ()
5437  +5.959 * deltaGmu() );
5438 
5439  } else if (Pol_em == 80. && Pol_ep == 0.){
5440  mu +=
5441  +121947. * CHbox / LambdaNP2
5442  +88774.4 * CHL1_11 / LambdaNP2
5443  -753269. * CHe_11 / LambdaNP2
5444  +88774.4 * CHL3_11 / LambdaNP2
5445  +54593.2 * CHD / LambdaNP2
5446  +2101955. * CHB / LambdaNP2
5447  +182237. * CHW / LambdaNP2
5448  +972861. * CHWB / LambdaNP2
5449  +29346.2 * CDHB / LambdaNP2
5450  -18562.1 * CDHW / LambdaNP2
5451  -0.206 * DeltaGF()
5452  ;
5453 
5454  // Add modifications due to small variations of the SM parameters
5455  mu += cHSM * ( -5.131 * deltaMz()
5456  -5.658 * deltaMh()
5457  +2.794 * deltaaMZ()
5458  +0.082 * deltaGmu() );
5459 
5460  } else if (Pol_em == -80. && Pol_ep == 0.){
5461  mu +=
5462  +122265. * CHbox / LambdaNP2
5463  +785643. * CHL1_11 / LambdaNP2
5464  -66907.6 * CHe_11 / LambdaNP2
5465  +785643. * CHL3_11 / LambdaNP2
5466  -107673. * CHD / LambdaNP2
5467  +1115316. * CHB / LambdaNP2
5468  +521873. * CHW / LambdaNP2
5469  -331727. * CHWB / LambdaNP2
5470  -32442.4 * CDHB / LambdaNP2
5471  +15348.7 * CDHW / LambdaNP2
5472  -5.334 * DeltaGF()
5473  ;
5474 
5475  // Add modifications due to small variations of the SM parameters
5476  mu += cHSM * ( +5.367 * deltaMz()
5477  -5.87 * deltaMh()
5478  -2.491 * deltaaMZ()
5479  +5.409 * deltaGmu() );
5480 
5481  } else {
5482  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5483  }
5484 
5485  } else if (sqrt_s == 0.250) {
5486 
5487  C1 = 0.0070;
5488 
5489  if (Pol_em == 80. && Pol_ep == -30.){
5490  mu +=
5491  +121054. * CHbox / LambdaNP2
5492  +51113. * CHL1_11 / LambdaNP2
5493  -851357. * CHe_11 / LambdaNP2
5494  +51113. * CHL3_11 / LambdaNP2
5495  +76762.9 * CHD / LambdaNP2
5496  +1629614. * CHB / LambdaNP2
5497  +72741.6 * CHW / LambdaNP2
5498  +1130834. * CHWB / LambdaNP2
5499  +34381.7 * CDHB / LambdaNP2
5500  -19876.5 * CDHW / LambdaNP2
5501  +0.563 * DeltaGF()
5502  ;
5503 
5504  // Add modifications due to small variations of the SM parameters
5505  mu += cHSM * ( -5.658 * deltaMz()
5506  -4.485 * deltaMh()
5507  +3.577 * deltaaMZ()
5508  -0.638 * deltaGmu() );
5509 
5510  } else if (Pol_em == -80. && Pol_ep == 30.){
5511  mu +=
5512  +121471. * CHbox / LambdaNP2
5513  +824294. * CHL1_11 / LambdaNP2
5514  -45066.5 * CHe_11 / LambdaNP2
5515  +824294. * CHL3_11 / LambdaNP2
5516  -128864. * CHD / LambdaNP2
5517  +644513. * CHB / LambdaNP2
5518  +425051. * CHW / LambdaNP2
5519  -383720. * CHWB / LambdaNP2
5520  -32434.3 * CDHB / LambdaNP2
5521  +15329.4 * CDHW / LambdaNP2
5522  -6.022 * DeltaGF()
5523  ;
5524 
5525  // Add modifications due to small variations of the SM parameters
5526  mu += cHSM * ( +7.852 * deltaMz()
5527  -4.536 * deltaMh()
5528  -3.165 * deltaaMZ()
5529  +6.136 * deltaGmu() );
5530 
5531  } else if (Pol_em == 80. && Pol_ep == 0.){
5532  mu +=
5533  +121494. * CHbox / LambdaNP2
5534  +77372.1 * CHL1_11 / LambdaNP2
5535  -676199. * CHe_11 / LambdaNP2
5536  +77372.1 * CHL3_11 / LambdaNP2
5537  +53294.7 * CHD / LambdaNP2
5538  +1668830. * CHB / LambdaNP2
5539  +145010. * CHW / LambdaNP2
5540  +772902. * CHWB / LambdaNP2
5541  +23910.6 * CDHB / LambdaNP2
5542  -16890.6 * CDHW / LambdaNP2
5543  -0.226 * DeltaGF()
5544  ;
5545 
5546  // Add modifications due to small variations of the SM parameters
5547  mu += cHSM * ( -4.183 * deltaMz()
5548  -4.557 * deltaMh()
5549  +2.773 * deltaaMZ()
5550  +0.148 * deltaGmu() );
5551 
5552  } else if (Pol_em == -80. && Pol_ep == 0.){
5553  mu +=
5554  +121947. * CHbox / LambdaNP2
5555  +713174. * CHL1_11 / LambdaNP2
5556  -53393.3 * CHe_11 / LambdaNP2
5557  +713174. * CHL3_11 / LambdaNP2
5558  -111120. * CHD / LambdaNP2
5559  +843388. * CHB / LambdaNP2
5560  +417838. * CHW / LambdaNP2
5561  -386753. * CHWB / LambdaNP2
5562  -27915.7 * CDHB / LambdaNP2
5563  +11946.5 * CDHW / LambdaNP2
5564  -5.496 * DeltaGF()
5565  ;
5566 
5567  // Add modifications due to small variations of the SM parameters
5568  mu += cHSM * ( +6.641 * deltaMz()
5569  -4.576 * deltaMh()
5570  -2.605 * deltaaMZ()
5571  +5.56 * deltaGmu() );
5572 
5573  } else {
5574  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5575  }
5576 
5577  } else if (sqrt_s == 0.350) {
5578 
5579  C1 = 0.0069;
5580 
5581  if (Pol_em == 80. && Pol_ep == -30.){
5582  mu +=
5583  +121674. * CHbox / LambdaNP2
5584  -47420.2 * CHL1_11 / LambdaNP2
5585  -172088. * CHe_11 / LambdaNP2
5586  -47420.2 * CHL3_11 / LambdaNP2
5587  +59728. * CHD / LambdaNP2
5588  +544205. * CHB / LambdaNP2
5589  +83604.4 * CHW / LambdaNP2
5590  +435393. * CHWB / LambdaNP2
5591  -24800.4 * CDHB / LambdaNP2
5592  -4583.09 * CDHW / LambdaNP2
5593  -0.05 * DeltaGF()
5594  ;
5595 
5596  // Add modifications due to small variations of the SM parameters
5597  mu += cHSM * ( -2.905 * deltaMz()
5598  -1.842 * deltaMh()
5599  +2.966 * deltaaMZ()
5600  +0.009 * deltaGmu() );
5601 
5602  } else if (Pol_em == -80. && Pol_ep == 30.){
5603  mu +=
5604  +121541. * CHbox / LambdaNP2
5605  +197618. * CHL1_11 / LambdaNP2
5606  +42238.9 * CHe_11 / LambdaNP2
5607  +197618. * CHL3_11 / LambdaNP2
5608  -124376. * CHD / LambdaNP2
5609  +181154. * CHB / LambdaNP2
5610  +195329. * CHW / LambdaNP2
5611  -505800. * CHWB / LambdaNP2
5612  +13082.6 * CDHB / LambdaNP2
5613  -26607.4 * CDHW / LambdaNP2
5614  -6.096 * DeltaGF()
5615  ;
5616 
5617  // Add modifications due to small variations of the SM parameters
5618  mu += cHSM * ( +9.303 * deltaMz()
5619  -1.82 * deltaMh()
5620  -3.105 * deltaaMZ()
5621  +6.071 * deltaGmu() );
5622 
5623  } else if (Pol_em == 80. && Pol_ep == 0.){
5624  mu +=
5625  +121760. * CHbox / LambdaNP2
5626  -62853. * CHL1_11 / LambdaNP2
5627  -83019.6 * CHe_11 / LambdaNP2
5628  -62853. * CHL3_11 / LambdaNP2
5629  +34395.4 * CHD / LambdaNP2
5630  +623389. * CHB / LambdaNP2
5631  +123932. * CHW / LambdaNP2
5632  +181789. * CHWB / LambdaNP2
5633  -20420. * CDHB / LambdaNP2
5634  -7820.42 * CDHW / LambdaNP2
5635  -0.875 * DeltaGF()
5636  ;
5637 
5638  // Add modifications due to small variations of the SM parameters
5639  mu += cHSM * ( -1.322 * deltaMz()
5640  -1.873 * deltaMh()
5641  +2.14 * deltaaMZ()
5642  +0.844 * deltaGmu() );
5643 
5644  } else if (Pol_em == -80. && Pol_ep == 0.){
5645  mu +=
5646  +121557. * CHbox / LambdaNP2
5647  +131443. * CHL1_11 / LambdaNP2
5648  +63326.7 * CHe_11 / LambdaNP2
5649  +131443. * CHL3_11 / LambdaNP2
5650  -103038. * CHD / LambdaNP2
5651  +323596. * CHB / LambdaNP2
5652  +201676. * CHW / LambdaNP2
5653  -491019. * CHWB / LambdaNP2
5654  +7992.43 * CDHB / LambdaNP2
5655  -24283.6 * CDHW / LambdaNP2
5656  -5.391 * DeltaGF()
5657  ;
5658 
5659  // Add modifications due to small variations of the SM parameters
5660  mu += cHSM * ( +7.818 * deltaMz()
5661  -1.846 * deltaMh()
5662  -2.402 * deltaaMZ()
5663  +5.358 * deltaGmu() );
5664 
5665  } else {
5666  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5667  }
5668 
5669  } else if (sqrt_s == 0.365) {
5670 
5671  C1 = 0.0069; // Use same as 350 GeV
5672 
5673  if (Pol_em == 80. && Pol_ep == -30.){
5674  mu +=
5675  +121458. * CHbox / LambdaNP2
5676  -58695.1 * CHL1_11 / LambdaNP2
5677  -109686. * CHe_11 / LambdaNP2
5678  -58695.1 * CHL3_11 / LambdaNP2
5679  +58496.7 * CHD / LambdaNP2
5680  +489137. * CHB / LambdaNP2
5681  +80751.3 * CHW / LambdaNP2
5682  +410304. * CHWB / LambdaNP2
5683  -30918.3 * CDHB / LambdaNP2
5684  -3571.31 * CDHW / LambdaNP2
5685  -0.085 * DeltaGF()
5686  ;
5687 
5688  // Add modifications due to small variations of the SM parameters
5689  mu += cHSM * ( -2.809 * deltaMz()
5690  -1.721 * deltaMh()
5691  +2.93 * deltaaMZ()
5692  +0.026 * deltaGmu() );
5693 
5694  } else if (Pol_em == -80. && Pol_ep == 30.){
5695  mu +=
5696  +121152. * CHbox / LambdaNP2
5697  +136019. * CHL1_11 / LambdaNP2
5698  +50762. * CHe_11 / LambdaNP2
5699  +136019. * CHL3_11 / LambdaNP2
5700  -123859. * CHD / LambdaNP2
5701  +165799. * CHB / LambdaNP2
5702  +176652. * CHW / LambdaNP2
5703  -504889. * CHWB / LambdaNP2
5704  +16920.7 * CDHB / LambdaNP2
5705  -31414.1 * CDHW / LambdaNP2
5706  -6.076 * DeltaGF()
5707  ;
5708 
5709  // Add modifications due to small variations of the SM parameters
5710  mu += cHSM * ( +9.271 * deltaMz()
5711  -1.7 * deltaMh()
5712  -3.092 * deltaaMZ()
5713  +6.031 * deltaGmu() );
5714 
5715  } else if (Pol_em == 80. && Pol_ep == 0.){
5716  mu +=
5717  +121193. * CHbox / LambdaNP2
5718  -76905.7 * CHL1_11 / LambdaNP2
5719  -32264.3 * CHe_11 / LambdaNP2
5720  -76905.7 * CHL3_11 / LambdaNP2
5721  +33650.3 * CHD / LambdaNP2
5722  +573505. * CHB / LambdaNP2
5723  +117937. * CHW / LambdaNP2
5724  +166382. * CHWB / LambdaNP2
5725  -25012.1 * CDHB / LambdaNP2
5726  -7703.47 * CDHW / LambdaNP2
5727  -0.911 * DeltaGF()
5728  ;
5729 
5730  // Add modifications due to small variations of the SM parameters
5731  mu += cHSM * ( -1.233 * deltaMz()
5732  -1.746 * deltaMh()
5733  +2.101 * deltaaMZ()
5734  +0.861 * deltaGmu() );
5735 
5736  } else if (Pol_em == -80. && Pol_ep == 0.){
5737  mu +=
5738  +121177. * CHbox / LambdaNP2
5739  +77981.5 * CHL1_11 / LambdaNP2
5740  +74274.1 * CHe_11 / LambdaNP2
5741  +77981.5 * CHL3_11 / LambdaNP2
5742  -102068. * CHD / LambdaNP2
5743  +305730. * CHB / LambdaNP2
5744  +183682. * CHW / LambdaNP2
5745  -487770. * CHWB / LambdaNP2
5746  +10624.8 * CDHB / LambdaNP2
5747  -28092.3 * CDHW / LambdaNP2
5748  -5.366 * DeltaGF()
5749  ;
5750 
5751  // Add modifications due to small variations of the SM parameters
5752  mu += cHSM * ( +7.791 * deltaMz()
5753  -1.726 * deltaMh()
5754  -2.377 * deltaaMZ()
5755  +5.325 * deltaGmu() );
5756 
5757  } else {
5758  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5759  }
5760 
5761  } else if (sqrt_s == 0.380) {
5762 
5763  C1 = 0.0069; // Use same as 350 GeV
5764 
5765  if (Pol_em == 80. && Pol_ep == -30.){
5766  mu +=
5767  +121392. * CHbox / LambdaNP2
5768  -68799.8 * CHL1_11 / LambdaNP2
5769  -54383.2 * CHe_11 / LambdaNP2
5770  -68799.8 * CHL3_11 / LambdaNP2
5771  +57427.7 * CHD / LambdaNP2
5772  +439155. * CHB / LambdaNP2
5773  +76978.2 * CHW / LambdaNP2
5774  +392293. * CHWB / LambdaNP2
5775  -36175.9 * CDHB / LambdaNP2
5776  -3193.74 * CDHW / LambdaNP2
5777  -0.11 * DeltaGF()
5778  ;
5779 
5780  // Add modifications due to small variations of the SM parameters
5781  mu += cHSM * ( -2.74 * deltaMz()
5782  -1.62 * deltaMh()
5783  +2.907 * deltaaMZ()
5784  +0.079 * deltaGmu() );
5785 
5786  } else if (Pol_em == -80. && Pol_ep == 30.){
5787  mu +=
5788  +121306. * CHbox / LambdaNP2
5789  +80159.7 * CHL1_11 / LambdaNP2
5790  +58002.2 * CHe_11 / LambdaNP2
5791  +80159.7 * CHL3_11 / LambdaNP2
5792  -123524. * CHD / LambdaNP2
5793  +151617. * CHB / LambdaNP2
5794  +154342. * CHW / LambdaNP2
5795  -500961. * CHWB / LambdaNP2
5796  +20509.9 * CDHB / LambdaNP2
5797  -35718.1 * CDHW / LambdaNP2
5798  -6.064 * DeltaGF()
5799  ;
5800 
5801  // Add modifications due to small variations of the SM parameters
5802  mu += cHSM * ( +9.254 * deltaMz()
5803  -1.608 * deltaMh()
5804  -3.07 * deltaaMZ()
5805  +6.04 * deltaGmu() );
5806 
5807  } else if (Pol_em == 80. && Pol_ep == 0.){
5808  mu +=
5809  +121171. * CHbox / LambdaNP2
5810  -89494.3 * CHL1_11 / LambdaNP2
5811  +11882.3 * CHe_11 / LambdaNP2
5812  -89494.3 * CHL3_11 / LambdaNP2
5813  +32430.1 * CHD / LambdaNP2
5814  +524620. * CHB / LambdaNP2
5815  +111520. * CHW / LambdaNP2
5816  +156122. * CHWB / LambdaNP2
5817  -29271.1 * CDHB / LambdaNP2
5818  -8056.8 * CDHW / LambdaNP2
5819  -0.928 * DeltaGF()
5820  ;
5821 
5822  // Add modifications due to small variations of the SM parameters
5823  mu += cHSM * ( -1.145 * deltaMz()
5824  -1.643 * deltaMh()
5825  +2.077 * deltaaMZ()
5826  +0.898 * deltaGmu() );
5827 
5828  } else if (Pol_em == -80. && Pol_ep == 0.){
5829  mu +=
5830  +121286. * CHbox / LambdaNP2
5831  +30046.7 * CHL1_11 / LambdaNP2
5832  +84014. * CHe_11 / LambdaNP2
5833  +30046.7 * CHL3_11 / LambdaNP2
5834  -101539. * CHD / LambdaNP2
5835  +286981. * CHB / LambdaNP2
5836  +164662. * CHW / LambdaNP2
5837  -480410. * CHWB / LambdaNP2
5838  +13149.6 * CDHB / LambdaNP2
5839  -31886.7 * CDHW / LambdaNP2
5840  -5.346 * DeltaGF()
5841  ;
5842 
5843  // Add modifications due to small variations of the SM parameters
5844  mu += cHSM * ( +7.766 * deltaMz()
5845  -1.629 * deltaMh()
5846  -2.353 * deltaaMZ()
5847  +5.316 * deltaGmu() );
5848 
5849  } else {
5850  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5851  }
5852 
5853  } else if (sqrt_s == 0.500) {
5854 
5855  C1 = 0.0067;
5856 
5857  if (Pol_em == 80. && Pol_ep == -30.){
5858  mu +=
5859  +121372. * CHbox / LambdaNP2
5860  -121062. * CHL1_11 / LambdaNP2
5861  +224754. * CHe_11 / LambdaNP2
5862  -121062. * CHL3_11 / LambdaNP2
5863  +55161.7 * CHD / LambdaNP2
5864  +201238. * CHB / LambdaNP2
5865  +52456.6 * CHW / LambdaNP2
5866  +335517. * CHWB / LambdaNP2
5867  -63733.4 * CDHB / LambdaNP2
5868  -2379.21 * CDHW / LambdaNP2
5869  -0.207 * DeltaGF()
5870  ;
5871 
5872  // Add modifications due to small variations of the SM parameters
5873  mu += cHSM * ( -2.453 * deltaMz()
5874  -1.136 * deltaMh()
5875  +2.81 * deltaaMZ()
5876  +0.175 * deltaGmu() );
5877 
5878  } else if (Pol_em == -80. && Pol_ep == 30.){
5879  mu +=
5880  +121399. * CHbox / LambdaNP2
5881  -200849. * CHL1_11 / LambdaNP2
5882  +96427.7 * CHe_11 / LambdaNP2
5883  -200849. * CHL3_11 / LambdaNP2
5884  -121178. * CHD / LambdaNP2
5885  +83220.9 * CHB / LambdaNP2
5886  +42832.2 * CHW / LambdaNP2
5887  -464173. * CHWB / LambdaNP2
5888  +37654.2 * CDHB / LambdaNP2
5889  -59029.6 * CDHW / LambdaNP2
5890  -6.025 * DeltaGF()
5891  ;
5892 
5893  // Add modifications due to small variations of the SM parameters
5894  mu += cHSM * ( +9.205 * deltaMz()
5895  -1.133 * deltaMh()
5896  -3.019 * deltaaMZ()
5897  +5.99 * deltaGmu() );
5898 
5899  } else if (Pol_em == 80. && Pol_ep == 0.){
5900  mu +=
5901  +121435. * CHbox / LambdaNP2
5902  -154953. * CHL1_11 / LambdaNP2
5903  +235326. * CHe_11 / LambdaNP2
5904  -154953. * CHL3_11 / LambdaNP2
5905  +30472. * CHD / LambdaNP2
5906  +298145. * CHB / LambdaNP2
5907  +75047.6 * CHW / LambdaNP2
5908  +137304. * CHWB / LambdaNP2
5909  -49636.1 * CDHB / LambdaNP2
5910  -10277.1 * CDHW / LambdaNP2
5911  -1.027 * DeltaGF()
5912  ;
5913 
5914  // Add modifications due to small variations of the SM parameters
5915  mu += cHSM * ( -0.829 * deltaMz()
5916  -1.142 * deltaMh()
5917  +1.988 * deltaaMZ()
5918  +0.989 * deltaGmu() );
5919 
5920  } else if (Pol_em == -80. && Pol_ep == 0.){
5921  mu +=
5922  +121468. * CHbox / LambdaNP2
5923  -208577. * CHL1_11 / LambdaNP2
5924  +134790. * CHe_11 / LambdaNP2
5925  -208577. * CHL3_11 / LambdaNP2
5926  -98708.1 * CHD / LambdaNP2
5927  +190310. * CHB / LambdaNP2
5928  +62321.4 * CHW / LambdaNP2
5929  -429412. * CHWB / LambdaNP2
5930  +24628.2 * CDHB / LambdaNP2
5931  -51722.9 * CDHW / LambdaNP2
5932  -5.287 * DeltaGF()
5933  ;
5934 
5935  // Add modifications due to small variations of the SM parameters
5936  mu += cHSM * ( +7.714 * deltaMz()
5937  -1.14 * deltaMh()
5938  -2.279 * deltaaMZ()
5939  +5.251 * deltaGmu() );
5940 
5941  } else {
5942  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
5943  }
5944 
5945  } else if (sqrt_s == 1.0) {
5946 
5947  C1 = 0.0065;
5948 
5949  if (Pol_em == 80. && Pol_ep == -30.){
5950  mu +=
5951  +121044. * CHbox / LambdaNP2
5952  -206156. * CHL1_11 / LambdaNP2
5953  +586357. * CHe_11 / LambdaNP2
5954  -206156. * CHL3_11 / LambdaNP2
5955  +54157.3 * CHD / LambdaNP2
5956  -30839.6 * CHB / LambdaNP2
5957  +18110.3 * CHW / LambdaNP2
5958  +345253. * CHWB / LambdaNP2
5959  -108488. * CDHB / LambdaNP2
5960  -12324.2 * CDHW / LambdaNP2
5961  -0.229 * DeltaGF()
5962  ;
5963 
5964  // Add modifications due to small variations of the SM parameters
5965  mu += cHSM * ( -2.141 * deltaMz()
5966  -0.544 * deltaMh()
5967  +2.775 * deltaaMZ()
5968  +0.211 * deltaGmu() );
5969 
5970  } else if (Pol_em == -80. && Pol_ep == 30.){
5971  mu +=
5972  +121085. * CHbox / LambdaNP2
5973  -565700. * CHL1_11 / LambdaNP2
5974  +157498. * CHe_11 / LambdaNP2
5975  -565700. * CHL3_11 / LambdaNP2
5976  -120795. * CHD / LambdaNP2
5977  +7953.6 * CHB / LambdaNP2
5978  -79908.9 * CHW / LambdaNP2
5979  -402278. * CHWB / LambdaNP2
5980  +54805.3 * CDHB / LambdaNP2
5981  -101988. * CDHW / LambdaNP2
5982  -6.001 * DeltaGF()
5983  ;
5984 
5985  // Add modifications due to small variations of the SM parameters
5986  mu += cHSM * ( +9.412 * deltaMz()
5987  -0.546 * deltaMh()
5988  -3.005 * deltaaMZ()
5989  +5.986 * deltaGmu() );
5990 
5991  } else if (Pol_em == 80. && Pol_ep == 0.){
5992  mu +=
5993  +120996. * CHbox / LambdaNP2
5994  -263143. * CHL1_11 / LambdaNP2
5995  +533190. * CHe_11 / LambdaNP2
5996  -263143. * CHL3_11 / LambdaNP2
5997  +29434.5 * CHD / LambdaNP2
5998  +63176.5 * CHB / LambdaNP2
5999  +26728.5 * CHW / LambdaNP2
6000  +184228. * CHWB / LambdaNP2
6001  -85487.1 * CDHB / LambdaNP2
6002  -24906.1 * CDHW / LambdaNP2
6003  -1.044 * DeltaGF()
6004  ;
6005 
6006  // Add modifications due to small variations of the SM parameters
6007  mu += cHSM * ( -0.508 * deltaMz()
6008  -0.545 * deltaMh()
6009  +1.958 * deltaaMZ()
6010  +1.027 * deltaGmu() );
6011 
6012  } else if (Pol_em == -80. && Pol_ep == 0.){
6013  mu +=
6014  +121114. * CHbox / LambdaNP2
6015  -524119. * CHL1_11 / LambdaNP2
6016  +218758. * CHe_11 / LambdaNP2
6017  -524119. * CHL3_11 / LambdaNP2
6018  -98164. * CHD / LambdaNP2
6019  +74694.7 * CHB / LambdaNP2
6020  -49060.4 * CHW / LambdaNP2
6021  -348619. * CHWB / LambdaNP2
6022  +33861.6 * CDHB / LambdaNP2
6023  -90369.8 * CDHW / LambdaNP2
6024  -5.256 * DeltaGF()
6025  ;
6026 
6027  // Add modifications due to small variations of the SM parameters
6028  mu += cHSM * ( +7.922 * deltaMz()
6029  -0.546 * deltaMh()
6030  -2.261 * deltaaMZ()
6031  +5.242 * deltaGmu() );
6032 
6033  } else {
6034  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6035  }
6036 
6037  } else if (sqrt_s == 1.4) {
6038 
6039  C1 = 0.0065;
6040 
6041  if (Pol_em == 80. && Pol_ep == -30.){
6042  mu +=
6043  +120762. * CHbox / LambdaNP2
6044  -242720. * CHL1_11 / LambdaNP2
6045  +714345. * CHe_11 / LambdaNP2
6046  -242720. * CHL3_11 / LambdaNP2
6047  +53823.3 * CHD / LambdaNP2
6048  -64876.7 * CHB / LambdaNP2
6049  +9362.37 * CHW / LambdaNP2
6050  +355440. * CHWB / LambdaNP2
6051  -127361. * CDHB / LambdaNP2
6052  -18147.3 * CDHW / LambdaNP2
6053  -0.228 * DeltaGF()
6054  ;
6055 
6056  // Add modifications due to small variations of the SM parameters
6057  mu += cHSM * ( -2.05 * deltaMz()
6058  -0.422 * deltaMh()
6059  +2.78 * deltaaMZ()
6060  +0.2 * deltaGmu() );
6061 
6062  } else if (Pol_em == -80. && Pol_ep == 30.){
6063  mu +=
6064  +120818. * CHbox / LambdaNP2
6065  -692905. * CHL1_11 / LambdaNP2
6066  +184416. * CHe_11 / LambdaNP2
6067  -692905. * CHL3_11 / LambdaNP2
6068  -121143. * CHD / LambdaNP2
6069  -4989.81 * CHB / LambdaNP2
6070  -93241.6 * CHW / LambdaNP2
6071  -392394. * CHWB / LambdaNP2
6072  +60556.9 * CDHB / LambdaNP2
6073  -121409. * CDHW / LambdaNP2
6074  -6.003 * DeltaGF()
6075  ;
6076 
6077  // Add modifications due to small variations of the SM parameters
6078  mu += cHSM * ( +9.501 * deltaMz()
6079  -0.422 * deltaMh()
6080  -2.999 * deltaaMZ()
6081  +5.972 * deltaGmu() );
6082 
6083  } else if (Pol_em == 80. && Pol_ep == 0.){
6084  mu +=
6085  +120773. * CHbox / LambdaNP2
6086  -309806. * CHL1_11 / LambdaNP2
6087  +643900. * CHe_11 / LambdaNP2
6088  -309806. * CHL3_11 / LambdaNP2
6089  +29091.1 * CHD / LambdaNP2
6090  +22438.3 * CHB / LambdaNP2
6091  +16021.7 * CHW / LambdaNP2
6092  +202496. * CHWB / LambdaNP2
6093  -100775. * CDHB / LambdaNP2
6094  -32830.8 * CDHW / LambdaNP2
6095  -1.043 * DeltaGF()
6096  ;
6097 
6098  // Add modifications due to small variations of the SM parameters
6099  mu += cHSM * ( -0.415 * deltaMz()
6100  -0.422 * deltaMh()
6101  +1.961 * deltaaMZ()
6102  +1.014 * deltaGmu() );
6103 
6104  } else if (Pol_em == -80. && Pol_ep == 0.){
6105  mu +=
6106  +120795. * CHbox / LambdaNP2
6107  -637584. * CHL1_11 / LambdaNP2
6108  +256188. * CHe_11 / LambdaNP2
6109  -637584. * CHL3_11 / LambdaNP2
6110  -98543.3 * CHD / LambdaNP2
6111  +49040.2 * CHB / LambdaNP2
6112  -63051.7 * CHW / LambdaNP2
6113  -332850. * CHWB / LambdaNP2
6114  +36510.1 * CDHB / LambdaNP2
6115  -108018. * CDHW / LambdaNP2
6116  -5.256 * DeltaGF()
6117  ;
6118 
6119  // Add modifications due to small variations of the SM parameters
6120  mu += cHSM * ( +8.01 * deltaMz()
6121  -0.423 * deltaMh()
6122  -2.255 * deltaaMZ()
6123  +5.227 * deltaGmu() );
6124 
6125  } else {
6126  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6127  }
6128 
6129  } else if (sqrt_s == 1.5) {
6130 
6131  C1 = 0.0065;// Use the same as 1400 GeV
6132 
6133  if (Pol_em == 80. && Pol_ep == -30.){
6134  mu +=
6135  +120570. * CHbox / LambdaNP2
6136  -250340. * CHL1_11 / LambdaNP2
6137  +739684. * CHe_11 / LambdaNP2
6138  -250340. * CHL3_11 / LambdaNP2
6139  +53685.8 * CHD / LambdaNP2
6140  -71192.9 * CHB / LambdaNP2
6141  +9743.41 * CHW / LambdaNP2
6142  +357556. * CHWB / LambdaNP2
6143  -131206. * CDHB / LambdaNP2
6144  -19448. * CDHW / LambdaNP2
6145  -0.224 * DeltaGF()
6146  ;
6147 
6148  // Add modifications due to small variations of the SM parameters
6149  mu += cHSM * ( -2.032 * deltaMz()
6150  -0.4 * deltaMh()
6151  +2.778 * deltaaMZ()
6152  +0.194 * deltaGmu() );
6153 
6154  } else if (Pol_em == -80. && Pol_ep == 30.){
6155  mu +=
6156  +120602. * CHbox / LambdaNP2
6157  -718001. * CHL1_11 / LambdaNP2
6158  +189852. * CHe_11 / LambdaNP2
6159  -718001. * CHL3_11 / LambdaNP2
6160  -121214. * CHD / LambdaNP2
6161  -6057.91 * CHB / LambdaNP2
6162  -95148.1 * CHW / LambdaNP2
6163  -390958. * CHWB / LambdaNP2
6164  +61690.7 * CDHB / LambdaNP2
6165  -125382. * CDHW / LambdaNP2
6166  -5.997 * DeltaGF()
6167  ;
6168 
6169  // Add modifications due to small variations of the SM parameters
6170  mu += cHSM * ( +9.519 * deltaMz()
6171  -0.399 * deltaMh()
6172  -3.001 * deltaaMZ()
6173  +5.965 * deltaGmu() );
6174 
6175  } else if (Pol_em == 80. && Pol_ep == 0.){
6176  mu +=
6177  +120563. * CHbox / LambdaNP2
6178  -319378. * CHL1_11 / LambdaNP2
6179  +665765. * CHe_11 / LambdaNP2
6180  -319378. * CHL3_11 / LambdaNP2
6181  +29010.7 * CHD / LambdaNP2
6182  +14190.4 * CHB / LambdaNP2
6183  +16080. * CHW / LambdaNP2
6184  +205187. * CHWB / LambdaNP2
6185  -103927. * CDHB / LambdaNP2
6186  -34420.2 * CDHW / LambdaNP2
6187  -1.04 * DeltaGF()
6188  ;
6189 
6190  // Add modifications due to small variations of the SM parameters
6191  mu += cHSM * ( -0.398 * deltaMz()
6192  -0.4 * deltaMh()
6193  +1.96 * deltaaMZ()
6194  +1.01 * deltaGmu() );
6195 
6196  } else if (Pol_em == -80. && Pol_ep == 0.){
6197  mu +=
6198  +120607. * CHbox / LambdaNP2
6199  -659879. * CHL1_11 / LambdaNP2
6200  +263841. * CHe_11 / LambdaNP2
6201  -659879. * CHL3_11 / LambdaNP2
6202  -98617.3 * CHD / LambdaNP2
6203  +46418.4 * CHB / LambdaNP2
6204  -64166.6 * CHW / LambdaNP2
6205  -330855. * CHWB / LambdaNP2
6206  +36774.5 * CDHB / LambdaNP2
6207  -111573. * CDHW / LambdaNP2
6208  -5.253 * DeltaGF()
6209  ;
6210 
6211  // Add modifications due to small variations of the SM parameters
6212  mu += cHSM * ( +8.03 * deltaMz()
6213  -0.4 * deltaMh()
6214  -2.257 * deltaaMZ()
6215  +5.221 * deltaGmu() );
6216 
6217  } else {
6218  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6219  }
6220 
6221  } else if (sqrt_s == 3.0) {
6222 
6223  C1 = 0.0063;
6224 
6225  if (Pol_em == 80. && Pol_ep == -30.){
6226  mu +=
6227  +120539. * CHbox / LambdaNP2
6228  -327096. * CHL1_11 / LambdaNP2
6229  +988310. * CHe_11 / LambdaNP2
6230  -327096. * CHL3_11 / LambdaNP2
6231  +53758.1 * CHD / LambdaNP2
6232  -79161. * CHB / LambdaNP2
6233  +3856.87 * CHW / LambdaNP2
6234  +369878. * CHWB / LambdaNP2
6235  -170059. * CDHB / LambdaNP2
6236  -32235.8 * CDHW / LambdaNP2
6237  -0.226 * DeltaGF()
6238  ;
6239 
6240  // Add modifications due to small variations of the SM parameters
6241  mu += cHSM * ( -1.896 * deltaMz()
6242  -0.264 * deltaMh()
6243  +2.778 * deltaaMZ()
6244  +0.174 * deltaGmu() );
6245 
6246  } else if (Pol_em == -80. && Pol_ep == 30.){
6247  mu +=
6248  +120565. * CHbox / LambdaNP2
6249  -961658. * CHL1_11 / LambdaNP2
6250  +247947. * CHe_11 / LambdaNP2
6251  -961658. * CHL3_11 / LambdaNP2
6252  -121230. * CHD / LambdaNP2
6253  -10752.9 * CHB / LambdaNP2
6254  -92123.7 * CHW / LambdaNP2
6255  -391807. * CHWB / LambdaNP2
6256  +73242.2 * CDHB / LambdaNP2
6257  -165690. * CDHW / LambdaNP2
6258  -6.002 * DeltaGF()
6259  ;
6260 
6261  // Add modifications due to small variations of the SM parameters
6262  mu += cHSM * ( +9.659 * deltaMz()
6263  -0.264 * deltaMh()
6264  -3.003 * deltaaMZ()
6265  +5.943 * deltaGmu() );
6266 
6267  } else if (Pol_em == 80. && Pol_ep == 0.){
6268  mu +=
6269  +120534. * CHbox / LambdaNP2
6270  -417962. * CHL1_11 / LambdaNP2
6271  +884851. * CHe_11 / LambdaNP2
6272  -417962. * CHL3_11 / LambdaNP2
6273  +29065.5 * CHD / LambdaNP2
6274  -10885.4 * CHB / LambdaNP2
6275  +8249.25 * CHW / LambdaNP2
6276  +228820. * CHWB / LambdaNP2
6277  -135851. * CDHB / LambdaNP2
6278  -51177.2 * CDHW / LambdaNP2
6279  -1.04 * DeltaGF()
6280  ;
6281 
6282  // Add modifications due to small variations of the SM parameters
6283  mu += cHSM * ( -0.262 * deltaMz()
6284  -0.264 * deltaMh()
6285  +1.959 * deltaaMZ()
6286  +0.987 * deltaGmu() );
6287 
6288  } else if (Pol_em == -80. && Pol_ep == 0.){
6289  mu +=
6290  +120480. * CHbox / LambdaNP2
6291  -880604. * CHL1_11 / LambdaNP2
6292  +344657. * CHe_11 / LambdaNP2
6293  -880604. * CHL3_11 / LambdaNP2
6294  -98656.8 * CHD / LambdaNP2
6295  +28681.4 * CHB / LambdaNP2
6296  -66216.6 * CHW / LambdaNP2
6297  -320715. * CHWB / LambdaNP2
6298  +41721.6 * CDHB / LambdaNP2
6299  -148698. * CDHW / LambdaNP2
6300  -5.256 * DeltaGF()
6301  ;
6302 
6303  // Add modifications due to small variations of the SM parameters
6304  mu += cHSM * ( +8.169 * deltaMz()
6305  -0.264 * deltaMh()
6306  -2.259 * deltaaMZ()
6307  +5.202 * deltaGmu() );
6308 
6309  } else {
6310  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6311  }
6312 
6313  } else
6314  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6315 
6316  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6317  //(Assume similar to WBF.)
6318  mu += eeeWBFint + eeeWBFpar;
6319 
6320 // Linear contribution from Higgs self-coupling
6321  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
6322 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
6324 
6325  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6326 
6327  return mu;
6328 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeZH()

double NPSMEFTd6::mueeZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 6895 of file NPSMEFTd6.cpp.

6896 {
6897  double mu = 1.0;
6898 
6899  double C1 = 0.0;
6900 
6901  if (sqrt_s == 0.240) {
6902 
6903  C1 = 0.017;
6904 
6905  mu +=
6906  +121263. * CHbox / LambdaNP2
6907  +898682. * CHL1_11 / LambdaNP2
6908  -767820. * CHe_11 / LambdaNP2
6909  +898682. * CHL3_11 / LambdaNP2
6910  -6046.36 * CHD / LambdaNP2
6911  +122439. * CHB / LambdaNP2
6912  +540057. * CHW / LambdaNP2
6913  +231063. * CHWB / LambdaNP2
6914  +17593.2 * CDHB / LambdaNP2
6915  +53409.5 * CDHW / LambdaNP2
6916  -2.2 * DeltaGF()
6917  ;
6918 
6919  // Add modifications due to small variations of the SM parameters
6920  mu += cHSM * ( -0.2 * deltaaMZ()
6921  +2.2 * deltaGmu()
6922  +4.775 * deltaMz()
6923  -3.071 * deltaMh() );
6924 
6925  if (FlagQuadraticTerms) {
6926  //Add contributions that are quadratic in the effective coefficients
6927  mu += 0.0;
6928  }
6929 
6930  } else if (sqrt_s == 0.250) {
6931 
6932  C1 = 0.015;
6933 
6934  mu +=
6935  +121263. * CHbox / LambdaNP2
6936  +975101. * CHL1_11 / LambdaNP2
6937  -833750. * CHe_11 / LambdaNP2
6938  +975101. * CHL3_11 / LambdaNP2
6939  -6046.36 * CHD / LambdaNP2
6940  +128443. * CHB / LambdaNP2
6941  +568273. * CHW / LambdaNP2
6942  +244206. * CHWB / LambdaNP2
6943  +19818.6 * CDHB / LambdaNP2
6944  +60127.6 * CDHW / LambdaNP2
6945  -2.2 * DeltaGF()
6946  ;
6947 
6948  // Add modifications due to small variations of the SM parameters
6949  mu += cHSM * ( -0.2 * deltaaMZ()
6950  +2.2 * deltaGmu()
6951  +5.219 * deltaMz()
6952  -2.27 * deltaMh() );
6953 
6954  if (FlagQuadraticTerms) {
6955  //Add contributions that are quadratic in the effective coefficients
6956  mu += 0.0;
6957  }
6958 
6959  } else if (sqrt_s == 0.350) {
6960 
6961  C1 = 0.0057;
6962 
6963  mu +=
6964  +121283. * CHbox / LambdaNP2
6965  +1911340. * CHL1_11 / LambdaNP2
6966  -1640958. * CHe_11 / LambdaNP2
6967  +1911340. * CHL3_11 / LambdaNP2
6968  -6009.52 * CHD / LambdaNP2
6969  +173183. * CHB / LambdaNP2
6970  +785843. * CHW / LambdaNP2
6971  +344494. * CHWB / LambdaNP2
6972  +59158.7 * CDHB / LambdaNP2
6973  +167954. * CDHW / LambdaNP2
6974  -2.201 * DeltaGF()
6975  ;
6976 
6977  // Add modifications due to small variations of the SM parameters
6978  mu += cHSM * ( -0.2 * deltaaMZ()
6979  +2.2 * deltaGmu()
6980  +5.396 * deltaMz()
6981  -0.729 * deltaMh() );
6982 
6983  if (FlagQuadraticTerms) {
6984  //Add contributions that are quadratic in the effective coefficients
6985  mu += 0.0;
6986  }
6987 
6988  } else if (sqrt_s == 0.365) {
6989 
6990  C1 = 0.0057; // Use same as 350 GeV
6991 
6992  mu +=
6993  +121243. * CHbox / LambdaNP2
6994  +2078482. * CHL1_11 / LambdaNP2
6995  -1785085. * CHe_11 / LambdaNP2
6996  +2078482. * CHL3_11 / LambdaNP2
6997  -6010.65 * CHD / LambdaNP2
6998  +178173. * CHB / LambdaNP2
6999  +809806. * CHW / LambdaNP2
7000  +355487. * CHWB / LambdaNP2
7001  +67662.7 * CDHB / LambdaNP2
7002  +190194. * CDHW / LambdaNP2
7003  -2.201 * DeltaGF()
7004  ;
7005 
7006  // Add modifications due to small variations of the SM parameters
7007  mu += cHSM * ( -0.2 * deltaaMZ()
7008  +2.2 * deltaGmu()
7009  +5.348 * deltaMz()
7010  -0.664 * deltaMh() );
7011 
7012  if (FlagQuadraticTerms) {
7013  //Add contributions that are quadratic in the effective coefficients
7014  mu += 0.0;
7015  }
7016 
7017  } else if (sqrt_s == 0.380) {
7018 
7019  C1 = 0.0057; // Use same as 350 GeV
7020 
7021  mu +=
7022  +121281. * CHbox / LambdaNP2
7023  +2253013. * CHL1_11 / LambdaNP2
7024  -1934557. * CHe_11 / LambdaNP2
7025  +2253013. * CHL3_11 / LambdaNP2
7026  -6026.37 * CHD / LambdaNP2
7027  +182674. * CHB / LambdaNP2
7028  +832109. * CHW / LambdaNP2
7029  +365819. * CHWB / LambdaNP2
7030  +76742. * CDHB / LambdaNP2
7031  +214030. * CDHW / LambdaNP2
7032  -2.202 * DeltaGF()
7033  ;
7034 
7035  // Add modifications due to small variations of the SM parameters
7036  mu += cHSM * ( -0.2 * deltaaMZ()
7037  +2.2 * deltaGmu()
7038  +5.301 * deltaMz()
7039  -0.609 * deltaMh() );
7040 
7041  if (FlagQuadraticTerms) {
7042  //Add contributions that are quadratic in the effective coefficients
7043  mu += 0.0;
7044  }
7045 
7046  } else if (sqrt_s == 0.500) {
7047 
7048  C1 = 0.00099;
7049 
7050  mu +=
7051  +121264. * CHbox / LambdaNP2
7052  +3900384. * CHL1_11 / LambdaNP2
7053  -3350136. * CHe_11 / LambdaNP2
7054  +3900384. * CHL3_11 / LambdaNP2
7055  -6019.22 * CHD / LambdaNP2
7056  +209229. * CHB / LambdaNP2
7057  +959942. * CHW / LambdaNP2
7058  +425112. * CHWB / LambdaNP2
7059  +169841. * CDHB / LambdaNP2
7060  +455437. * CDHW / LambdaNP2
7061  -2.202 * DeltaGF()
7062  ;
7063 
7064  // Add modifications due to small variations of the SM parameters
7065  mu += cHSM * ( -0.2 * deltaaMZ()
7066  +2.2 * deltaGmu()
7067  +5. * deltaMz()
7068  -0.351 * deltaMh() );
7069 
7070  if (FlagQuadraticTerms) {
7071  //Add contributions that are quadratic in the effective coefficients
7072  mu += 0.0;
7073  }
7074 
7075  } else if (sqrt_s == 1.0) {
7076 
7077  C1 = -0.0012;
7078 
7079  mu +=
7080  +121274. * CHbox / LambdaNP2
7081  +15601820. * CHL1_11 / LambdaNP2
7082  -13395670. * CHe_11 / LambdaNP2
7083  +15601820. * CHL3_11 / LambdaNP2
7084  -6040.16 * CHD / LambdaNP2
7085  +243960. * CHB / LambdaNP2
7086  +1128805. * CHW / LambdaNP2
7087  +503138. * CHWB / LambdaNP2
7088  +899357. * CDHB / LambdaNP2
7089  +2321619. * CDHW / LambdaNP2
7090  -2.202 * DeltaGF()
7091  ;
7092 
7093  // Add modifications due to small variations of the SM parameters
7094  mu += cHSM * ( -0.2 * deltaaMZ()
7095  +2.2 * deltaGmu()
7096  +4.574 * deltaMz()
7097  -0.092 * deltaMh() );
7098 
7099  if (FlagQuadraticTerms) {
7100  //Add contributions that are quadratic in the effective coefficients
7101  mu += 0.0;
7102  }
7103 
7104  } else if (sqrt_s == 1.4) {
7105 
7106  C1 = -0.0011;
7107 
7108  mu +=
7109  +121283. * CHbox / LambdaNP2
7110  +30579278. * CHL1_11 / LambdaNP2
7111  -26253064. * CHe_11 / LambdaNP2
7112  +30579278. * CHL3_11 / LambdaNP2
7113  -6010.77 * CHD / LambdaNP2
7114  +250804. * CHB / LambdaNP2
7115  +1161208. * CHW / LambdaNP2
7116  +518040. * CHWB / LambdaNP2
7117  +1848758. * CDHB / LambdaNP2
7118  +4747422. * CDHW / LambdaNP2
7119  -2.203 * DeltaGF()
7120  ;
7121 
7122  // Add modifications due to small variations of the SM parameters
7123  mu += cHSM * ( -0.2 * deltaaMZ()
7124  +2.2 * deltaGmu()
7125  +4.491 * deltaMz()
7126  -0.047 * deltaMh() );
7127 
7128  if (FlagQuadraticTerms) {
7129  //Add contributions that are quadratic in the effective coefficients
7130  mu += 0.0;
7131  }
7132 
7133  } else if (sqrt_s == 1.5) {
7134 
7135  C1 = -0.0011;// Use the same as 1400 GeV
7136 
7137  mu +=
7138  +121262. * CHbox / LambdaNP2
7139  +35102329. * CHL1_11 / LambdaNP2
7140  -30135878. * CHe_11 / LambdaNP2
7141  +35102329. * CHL3_11 / LambdaNP2
7142  -6034.22 * CHD / LambdaNP2
7143  +251576. * CHB / LambdaNP2
7144  +1165634. * CHW / LambdaNP2
7145  +519954. * CHWB / LambdaNP2
7146  +2132554. * CDHB / LambdaNP2
7147  +5481906. * CDHW / LambdaNP2
7148  -2.203 * DeltaGF()
7149  ;
7150 
7151  // Add modifications due to small variations of the SM parameters
7152  mu += cHSM * ( -0.2 * deltaaMZ()
7153  +2.2 * deltaGmu()
7154  +4.479 * deltaMz()
7155  -0.041 * deltaMh() );
7156 
7157  if (FlagQuadraticTerms) {
7158  //Add contributions that are quadratic in the effective coefficients
7159  mu += 0.0;
7160  }
7161 
7162  } else if (sqrt_s == 3.0) {
7163 
7164  C1 = -0.00054;
7165 
7166  mu +=
7167  +121279. * CHbox / LambdaNP2
7168  +140413697. * CHL1_11 / LambdaNP2
7169  -120540988. * CHe_11 / LambdaNP2
7170  +140413697. * CHL3_11 / LambdaNP2
7171  -6012.61 * CHD / LambdaNP2
7172  +257222. * CHB / LambdaNP2
7173  +1188444. * CHW / LambdaNP2
7174  +530503. * CHWB / LambdaNP2
7175  +8839419. * CDHB / LambdaNP2
7176  +22583370. * CDHW / LambdaNP2
7177  -2.202 * DeltaGF()
7178  ;
7179 
7180  // Add modifications due to small variations of the SM parameters
7181  mu += cHSM * ( -0.2 * deltaaMZ()
7182  +2.2 * deltaGmu()
7183  +4.42 * deltaMz()
7184  -0.01 * deltaMh() );
7185 
7186  if (FlagQuadraticTerms) {
7187  //Add contributions that are quadratic in the effective coefficients
7188  mu += 0.0;
7189  }
7190 
7191  } else
7192  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZH()");
7193 
7194  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7195  mu += eeeZHint + eeeZHpar;
7196 
7197 // Linear contribution from Higgs self-coupling
7198  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7199 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7201 
7202  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7203 
7204  return mu;
7205 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3649
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3648
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeZHPol()

double NPSMEFTd6::mueeZHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 7252 of file NPSMEFTd6.cpp.

7253 {
7254  double mu = 1.0;
7255 
7256  double C1 = 0.0;
7257 
7258  if (sqrt_s == 0.240) {
7259 
7260  C1 = 0.017;
7261 
7262  if (Pol_em == 80. && Pol_ep == -30.){
7263  mu +=
7264  +121260. * CHbox / LambdaNP2
7265  +117191. * CHL1_11 / LambdaNP2
7266  -1681596. * CHe_11 / LambdaNP2
7267  +117191. * CHL3_11 / LambdaNP2
7268  +74555.1 * CHD / LambdaNP2
7269  +528105. * CHB / LambdaNP2
7270  +134403. * CHW / LambdaNP2
7271  +872560. * CHWB / LambdaNP2
7272  +137571. * CDHB / LambdaNP2
7273  -12321.5 * CDHW / LambdaNP2
7274  +0.459 * DeltaGF()
7275  ;
7276 
7277  // Add modifications due to small variations of the SM parameters
7278  mu += cHSM * ( +2.46 * deltaaMZ()
7279  -0.46 * deltaGmu()
7280  -0.544 * deltaMz()
7281  -3.071 * deltaMh() );
7282 
7283  } else if (Pol_em == -80. && Pol_ep == 30.){
7284  mu +=
7285  +121254. * CHbox / LambdaNP2
7286  +1495015. * CHL1_11 / LambdaNP2
7287  -76567.2 * CHe_11 / LambdaNP2
7288  +1495015. * CHL3_11 / LambdaNP2
7289  -67582.1 * CHD / LambdaNP2
7290  -187104. * CHB / LambdaNP2
7291  +849552. * CHW / LambdaNP2
7292  -258537. * CHWB / LambdaNP2
7293  -73970.1 * CDHB / LambdaNP2
7294  +103582. * CDHW / LambdaNP2
7295  -4.23 * DeltaGF()
7296  ;
7297 
7298  // Add modifications due to small variations of the SM parameters
7299  mu += cHSM * ( -2.23 * deltaaMZ()
7300  +4.23 * deltaGmu()
7301  +8.834 * deltaMz()
7302  -3.071 * deltaMh() );
7303 
7304  } else if (Pol_em == 80. && Pol_ep == 0.){
7305  mu +=
7306  +121256. * CHbox / LambdaNP2
7307  +204529. * CHL1_11 / LambdaNP2
7308  -1578998. * CHe_11 / LambdaNP2
7309  +204529. * CHL3_11 / LambdaNP2
7310  +65548.7 * CHD / LambdaNP2
7311  +482729. * CHB / LambdaNP2
7312  +179733. * CHW / LambdaNP2
7313  +800870. * CHWB / LambdaNP2
7314  +124170. * CDHB / LambdaNP2
7315  -5016.48 * CDHW / LambdaNP2
7316  +0.162 * DeltaGF()
7317  ;
7318 
7319  // Add modifications due to small variations of the SM parameters
7320  mu += cHSM * ( +2.163 * deltaaMZ()
7321  -0.163 * deltaGmu()
7322  +0.05 * deltaMz()
7323  -3.071 * deltaMh() );
7324 
7325  } else if (Pol_em == -80. && Pol_ep == 0.){
7326  mu +=
7327  +121264. * CHbox / LambdaNP2
7328  +1442776. * CHL1_11 / LambdaNP2
7329  -137405. * CHe_11 / LambdaNP2
7330  +1442776. * CHL3_11 / LambdaNP2
7331  -62167.6 * CHD / LambdaNP2
7332  -159988. * CHB / LambdaNP2
7333  +822448. * CHW / LambdaNP2
7334  -215639. * CHWB / LambdaNP2
7335  -65950.1 * CDHB / LambdaNP2
7336  +99206.1 * CDHW / LambdaNP2
7337  -4.052 * DeltaGF()
7338  ;
7339 
7340  // Add modifications due to small variations of the SM parameters
7341  mu += cHSM * ( -2.052 * deltaaMZ()
7342  +4.052 * deltaGmu()
7343  +8.479 * deltaMz()
7344  -3.071 * deltaMh() );
7345 
7346  } else {
7347  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7348  }
7349 
7350  } else if (sqrt_s == 0.250) {
7351 
7352  C1 = 0.015;
7353 
7354  if (Pol_em == 80. && Pol_ep == -30.){
7355  mu +=
7356  +121264. * CHbox / LambdaNP2
7357  +127210. * CHL1_11 / LambdaNP2
7358  -1824910. * CHe_11 / LambdaNP2
7359  +127210. * CHL3_11 / LambdaNP2
7360  +74597.1 * CHD / LambdaNP2
7361  +560319. * CHB / LambdaNP2
7362  +136129. * CHW / LambdaNP2
7363  +902676. * CHWB / LambdaNP2
7364  +154358. * CDHB / LambdaNP2
7365  -13612.9 * CDHW / LambdaNP2
7366  +0.459 * DeltaGF()
7367  ;
7368 
7369  // Add modifications due to small variations of the SM parameters
7370  mu += cHSM * ( +2.46 * deltaaMZ()
7371  -0.46 * deltaGmu()
7372  -0.1 * deltaMz()
7373  -2.27 * deltaMh() );
7374 
7375  } else if (Pol_em == -80. && Pol_ep == 30.){
7376  mu +=
7377  +121257. * CHbox / LambdaNP2
7378  +1622228. * CHL1_11 / LambdaNP2
7379  -83107. * CHe_11 / LambdaNP2
7380  +1622228. * CHL3_11 / LambdaNP2
7381  -67554.3 * CHD / LambdaNP2
7382  -201409. * CHB / LambdaNP2
7383  +898116. * CHW / LambdaNP2
7384  -258306. * CHWB / LambdaNP2
7385  -82898. * CDHB / LambdaNP2
7386  +116421. * CDHW / LambdaNP2
7387  -4.23 * DeltaGF()
7388  ;
7389 
7390  // Add modifications due to small variations of the SM parameters
7391  mu += cHSM * ( -2.23 * deltaaMZ()
7392  +4.23 * deltaGmu()
7393  +9.279 * deltaMz()
7394  -2.27 * deltaMh() );
7395 
7396  } else if (Pol_em == 80. && Pol_ep == 0.){
7397  mu +=
7398  +121309. * CHbox / LambdaNP2
7399  +221930. * CHL1_11 / LambdaNP2
7400  -1714047. * CHe_11 / LambdaNP2
7401  +221930. * CHL3_11 / LambdaNP2
7402  +65599.6 * CHD / LambdaNP2
7403  +512136. * CHB / LambdaNP2
7404  +184424. * CHW / LambdaNP2
7405  +829145. * CHWB / LambdaNP2
7406  +139369. * CDHB / LambdaNP2
7407  -5351.17 * CDHW / LambdaNP2
7408  +0.162 * DeltaGF()
7409  ;
7410 
7411  // Add modifications due to small variations of the SM parameters
7412  mu += cHSM * ( +2.163 * deltaaMZ()
7413  -0.163 * deltaGmu()
7414  +0.494 * deltaMz()
7415  -2.27 * deltaMh() );
7416 
7417  } else if (Pol_em == -80. && Pol_ep == 0.){
7418  mu +=
7419  +121269. * CHbox / LambdaNP2
7420  +1565559. * CHL1_11 / LambdaNP2
7421  -148908. * CHe_11 / LambdaNP2
7422  +1565559. * CHL3_11 / LambdaNP2
7423  -62170. * CHD / LambdaNP2
7424  -172540. * CHB / LambdaNP2
7425  +869218. * CHW / LambdaNP2
7426  -214299. * CHWB / LambdaNP2
7427  -73929.8 * CDHB / LambdaNP2
7428  +111494. * CDHW / LambdaNP2
7429  -4.053 * DeltaGF()
7430  ;
7431 
7432  // Add modifications due to small variations of the SM parameters
7433  mu += cHSM * ( -2.052 * deltaaMZ()
7434  +4.052 * deltaGmu()
7435  +8.923 * deltaMz()
7436  -2.27 * deltaMh() );
7437 
7438  } else {
7439  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7440  }
7441 
7442  } else if (sqrt_s == 0.350) {
7443 
7444  C1 = 0.0057;
7445 
7446  if (Pol_em == 80. && Pol_ep == -30.){
7447  mu +=
7448  +121274. * CHbox / LambdaNP2
7449  +249309. * CHL1_11 / LambdaNP2
7450  -3576996. * CHe_11 / LambdaNP2
7451  +249309. * CHL3_11 / LambdaNP2
7452  +74596.5 * CHD / LambdaNP2
7453  +812491. * CHB / LambdaNP2
7454  +146212. * CHW / LambdaNP2
7455  +1135161. * CHWB / LambdaNP2
7456  +395085. * CDHB / LambdaNP2
7457  -16140.8 * CDHW / LambdaNP2
7458  +0.458 * DeltaGF()
7459  ;
7460 
7461  // Add modifications due to small variations of the SM parameters
7462  mu += cHSM * ( +2.46 * deltaaMZ()
7463  -0.46 * deltaGmu()
7464  +0.077 * deltaMz()
7465  -0.729 * deltaMh() );
7466 
7467  } else if (Pol_em == -80. && Pol_ep == 30.){
7468  mu +=
7469  +121289. * CHbox / LambdaNP2
7470  +3179548. * CHL1_11 / LambdaNP2
7471  -163347. * CHe_11 / LambdaNP2
7472  +3179548. * CHL3_11 / LambdaNP2
7473  -67524.8 * CHD / LambdaNP2
7474  -314653. * CHB / LambdaNP2
7475  +1273817. * CHW / LambdaNP2
7476  -258947. * CHWB / LambdaNP2
7477  -197137. * CDHB / LambdaNP2
7478  +308384. * CDHW / LambdaNP2
7479  -4.231 * DeltaGF()
7480  ;
7481 
7482  // Add modifications due to small variations of the SM parameters
7483  mu += cHSM * ( -2.23 * deltaaMZ()
7484  +4.23 * deltaGmu()
7485  +9.456 * deltaMz()
7486  -0.729 * deltaMh() );
7487 
7488  } else if (Pol_em == 80. && Pol_ep == 0.){
7489  mu +=
7490  +121304. * CHbox / LambdaNP2
7491  +434952. * CHL1_11 / LambdaNP2
7492  -3360980. * CHe_11 / LambdaNP2
7493  +434952. * CHL3_11 / LambdaNP2
7494  +65624.7 * CHD / LambdaNP2
7495  +741142. * CHB / LambdaNP2
7496  +217654. * CHW / LambdaNP2
7497  +1046799. * CHWB / LambdaNP2
7498  +357606. * CDHB / LambdaNP2
7499  +4440.1 * CDHW / LambdaNP2
7500  +0.161 * DeltaGF()
7501  ;
7502 
7503  // Add modifications due to small variations of the SM parameters
7504  mu += cHSM * ( +2.163 * deltaaMZ()
7505  -0.163 * deltaGmu()
7506  +0.671 * deltaMz()
7507  -0.729 * deltaMh() );
7508 
7509  } else if (Pol_em == -80. && Pol_ep == 0.){
7510  mu +=
7511  +121259. * CHbox / LambdaNP2
7512  +3068356. * CHL1_11 / LambdaNP2
7513  -292427. * CHe_11 / LambdaNP2
7514  +3068356. * CHL3_11 / LambdaNP2
7515  -62160.7 * CHD / LambdaNP2
7516  -271962. * CHB / LambdaNP2
7517  +1231171. * CHW / LambdaNP2
7518  -206112. * CHWB / LambdaNP2
7519  -174718. * CDHB / LambdaNP2
7520  +296046. * CDHW / LambdaNP2
7521  -4.053 * DeltaGF()
7522  ;
7523 
7524  // Add modifications due to small variations of the SM parameters
7525  mu += cHSM * ( -2.052 * deltaaMZ()
7526  +4.052 * deltaGmu()
7527  +9.1 * deltaMz()
7528  -0.729 * deltaMh() );
7529 
7530  } else {
7531  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7532  }
7533 
7534  } else if (sqrt_s == 0.365) {
7535 
7536  C1 = 0.0057; // Use same as 350 GeV
7537 
7538  if (Pol_em == 80. && Pol_ep == -30.){
7539  mu +=
7540  +121270. * CHbox / LambdaNP2
7541  +271098. * CHL1_11 / LambdaNP2
7542  -3890169. * CHe_11 / LambdaNP2
7543  +271098. * CHL3_11 / LambdaNP2
7544  +74554. * CHD / LambdaNP2
7545  +840573. * CHB / LambdaNP2
7546  +147108. * CHW / LambdaNP2
7547  +1160947. * CHWB / LambdaNP2
7548  +442125. * CDHB / LambdaNP2
7549  -15038.8 * CDHW / LambdaNP2
7550  +0.459 * DeltaGF()
7551  ;
7552 
7553  // Add modifications due to small variations of the SM parameters
7554  mu += cHSM * ( +2.46 * deltaaMZ()
7555  -0.46 * deltaGmu()
7556  +0.029 * deltaMz()
7557  -0.664 * deltaMh() );
7558 
7559  } else if (Pol_em == -80. && Pol_ep == 30.){
7560  mu +=
7561  +121238. * CHbox / LambdaNP2
7562  +3457848. * CHL1_11 / LambdaNP2
7563  -177584. * CHe_11 / LambdaNP2
7564  +3457848. * CHL3_11 / LambdaNP2
7565  -67578.3 * CHD / LambdaNP2
7566  -327391. * CHB / LambdaNP2
7567  +1315671. * CHW / LambdaNP2
7568  -259142. * CHWB / LambdaNP2
7569  -218241. * CDHB / LambdaNP2
7570  +346804. * CDHW / LambdaNP2
7571  -4.231 * DeltaGF()
7572  ;
7573 
7574  // Add modifications due to small variations of the SM parameters
7575  mu += cHSM * ( -2.23 * deltaaMZ()
7576  +4.23 * deltaGmu()
7577  +9.408 * deltaMz()
7578  -0.664 * deltaMh() );
7579 
7580  } else if (Pol_em == 80. && Pol_ep == 0.){
7581  mu +=
7582  +121251. * CHbox / LambdaNP2
7583  +472985. * CHL1_11 / LambdaNP2
7584  -3655203. * CHe_11 / LambdaNP2
7585  +472985. * CHL3_11 / LambdaNP2
7586  +65559.4 * CHD / LambdaNP2
7587  +766585. * CHB / LambdaNP2
7588  +221202. * CHW / LambdaNP2
7589  +1070933. * CHWB / LambdaNP2
7590  +400293. * CDHB / LambdaNP2
7591  +7914.02 * CDHW / LambdaNP2
7592  +0.161 * DeltaGF()
7593  ;
7594 
7595  // Add modifications due to small variations of the SM parameters
7596  mu += cHSM * ( +2.163 * deltaaMZ()
7597  -0.163 * deltaGmu()
7598  +0.623 * deltaMz()
7599  -0.664 * deltaMh() );
7600 
7601  } else if (Pol_em == -80. && Pol_ep == 0.){
7602  mu +=
7603  +121238. * CHbox / LambdaNP2
7604  +3336984. * CHL1_11 / LambdaNP2
7605  -317944. * CHe_11 / LambdaNP2
7606  +3336984. * CHL3_11 / LambdaNP2
7607  -62188.9 * CHD / LambdaNP2
7608  -283174. * CHB / LambdaNP2
7609  +1271272. * CHW / LambdaNP2
7610  -205330. * CHWB / LambdaNP2
7611  -193153. * CDHB / LambdaNP2
7612  +333078. * CDHW / LambdaNP2
7613  -4.053 * DeltaGF()
7614  ;
7615 
7616  // Add modifications due to small variations of the SM parameters
7617  mu += cHSM * ( -2.052 * deltaaMZ()
7618  +4.052 * deltaGmu()
7619  +9.052 * deltaMz()
7620  -0.664 * deltaMh() );
7621 
7622  } else {
7623  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7624  }
7625 
7626  } else if (sqrt_s == 0.380) {
7627 
7628  C1 = 0.0057; // Use same as 350 GeV
7629 
7630  if (Pol_em == 80. && Pol_ep == -30.){
7631  mu +=
7632  +121228. * CHbox / LambdaNP2
7633  +293860. * CHL1_11 / LambdaNP2
7634  -4216491. * CHe_11 / LambdaNP2
7635  +293860. * CHL3_11 / LambdaNP2
7636  +74561.4 * CHD / LambdaNP2
7637  +866754. * CHB / LambdaNP2
7638  +147982. * CHW / LambdaNP2
7639  +1184912. * CHWB / LambdaNP2
7640  +492018. * CDHB / LambdaNP2
7641  -13596.5 * CDHW / LambdaNP2
7642  +0.459 * DeltaGF()
7643  ;
7644 
7645  // Add modifications due to small variations of the SM parameters
7646  mu += cHSM * ( +2.46 * deltaaMZ()
7647  -0.46 * deltaGmu()
7648  -0.018 * deltaMz()
7649  -0.609 * deltaMh() );
7650 
7651  } else if (Pol_em == -80. && Pol_ep == 30.){
7652  mu +=
7653  +121226. * CHbox / LambdaNP2
7654  +3747707. * CHL1_11 / LambdaNP2
7655  -192650. * CHe_11 / LambdaNP2
7656  +3747707. * CHL3_11 / LambdaNP2
7657  -67608.3 * CHD / LambdaNP2
7658  -339193. * CHB / LambdaNP2
7659  +1354040. * CHW / LambdaNP2
7660  -259321. * CHWB / LambdaNP2
7661  -240311. * CDHB / LambdaNP2
7662  +387710. * CDHW / LambdaNP2
7663  -4.23 * DeltaGF()
7664  ;
7665 
7666  // Add modifications due to small variations of the SM parameters
7667  mu += cHSM * ( -2.23 * deltaaMZ()
7668  +4.23 * deltaGmu()
7669  +9.361 * deltaMz()
7670  -0.609 * deltaMh() );
7671 
7672  } else if (Pol_em == 80. && Pol_ep == 0.){
7673  mu +=
7674  +121325. * CHbox / LambdaNP2
7675  +512707. * CHL1_11 / LambdaNP2
7676  -3961665. * CHe_11 / LambdaNP2
7677  +512707. * CHL3_11 / LambdaNP2
7678  +65601.7 * CHD / LambdaNP2
7679  +790306. * CHB / LambdaNP2
7680  +224394. * CHW / LambdaNP2
7681  +1093297. * CHWB / LambdaNP2
7682  +445530. * CDHB / LambdaNP2
7683  +11860.4 * CDHW / LambdaNP2
7684  +0.161 * DeltaGF()
7685  ;
7686 
7687  // Add modifications due to small variations of the SM parameters
7688  mu += cHSM * ( +2.163 * deltaaMZ()
7689  -0.163 * deltaGmu()
7690  +0.576 * deltaMz()
7691  -0.609 * deltaMh() );
7692 
7693  } else if (Pol_em == -80. && Pol_ep == 0.){
7694  mu +=
7695  +121273. * CHbox / LambdaNP2
7696  +3617032. * CHL1_11 / LambdaNP2
7697  -344629. * CHe_11 / LambdaNP2
7698  +3617032. * CHL3_11 / LambdaNP2
7699  -62148.3 * CHD / LambdaNP2
7700  -293491. * CHB / LambdaNP2
7701  +1308558. * CHW / LambdaNP2
7702  -204594. * CHWB / LambdaNP2
7703  -212514. * CDHB / LambdaNP2
7704  +372554. * CDHW / LambdaNP2
7705  -4.053 * DeltaGF()
7706  ;
7707 
7708  // Add modifications due to small variations of the SM parameters
7709  mu += cHSM * ( -2.052 * deltaaMZ()
7710  +4.052 * deltaGmu()
7711  +9.005 * deltaMz()
7712  -0.609 * deltaMh() );
7713 
7714  } else {
7715  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7716  }
7717 
7718  } else if (sqrt_s == 0.500) {
7719 
7720  C1 = 0.00099;
7721 
7722  if (Pol_em == 80. && Pol_ep == -30.){
7723  mu +=
7724  +121268. * CHbox / LambdaNP2
7725  +508715. * CHL1_11 / LambdaNP2
7726  -7299333. * CHe_11 / LambdaNP2
7727  +508715. * CHL3_11 / LambdaNP2
7728  +74603.6 * CHD / LambdaNP2
7729  +1018069. * CHB / LambdaNP2
7730  +151257. * CHW / LambdaNP2
7731  +1323862. * CHWB / LambdaNP2
7732  +985604. * CDHB / LambdaNP2
7733  +8362.16 * CDHW / LambdaNP2
7734  +0.458 * DeltaGF()
7735  ;
7736 
7737  // Add modifications due to small variations of the SM parameters
7738  mu += cHSM * ( +2.46 * deltaaMZ()
7739  -0.46 * deltaGmu()
7740  -0.319 * deltaMz()
7741  -0.351 * deltaMh() );
7742 
7743  } else if (Pol_em == -80. && Pol_ep == 30.){
7744  mu +=
7745  +121273. * CHbox / LambdaNP2
7746  +6488707. * CHL1_11 / LambdaNP2
7747  -332950. * CHe_11 / LambdaNP2
7748  +6488707. * CHL3_11 / LambdaNP2
7749  -67530.9 * CHD / LambdaNP2
7750  -408101. * CHB / LambdaNP2
7751  +1576859. * CHW / LambdaNP2
7752  -260777. * CHWB / LambdaNP2
7753  -452746. * CDHB / LambdaNP2
7754  +796569. * CDHW / LambdaNP2
7755  -4.231 * DeltaGF()
7756  ;
7757 
7758  // Add modifications due to small variations of the SM parameters
7759  mu += cHSM * ( -2.23 * deltaaMZ()
7760  +4.23 * deltaGmu()
7761  +9.06 * deltaMz()
7762  -0.351 * deltaMh() );
7763 
7764  } else if (Pol_em == 80. && Pol_ep == 0.){
7765  mu +=
7766  +121280. * CHbox / LambdaNP2
7767  +887632. * CHL1_11 / LambdaNP2
7768  -6858533. * CHe_11 / LambdaNP2
7769  +887632. * CHL3_11 / LambdaNP2
7770  +65606.6 * CHD / LambdaNP2
7771  +927745. * CHB / LambdaNP2
7772  +241619. * CHW / LambdaNP2
7773  +1223535. * CHWB / LambdaNP2
7774  +894441. * CDHB / LambdaNP2
7775  +58317. * CDHW / LambdaNP2
7776  +0.161 * DeltaGF()
7777  ;
7778 
7779  // Add modifications due to small variations of the SM parameters
7780  mu += cHSM * ( +2.163 * deltaaMZ()
7781  -0.163 * deltaGmu()
7782  +0.275 * deltaMz()
7783  -0.351 * deltaMh() );
7784 
7785  } else if (Pol_em == -80. && Pol_ep == 0.){
7786  mu +=
7787  +121268. * CHbox / LambdaNP2
7788  +6262095. * CHL1_11 / LambdaNP2
7789  -597046. * CHe_11 / LambdaNP2
7790  +6262095. * CHL3_11 / LambdaNP2
7791  -62148.8 * CHD / LambdaNP2
7792  -353914. * CHB / LambdaNP2
7793  +1522841. * CHW / LambdaNP2
7794  -200684. * CHWB / LambdaNP2
7795  -398214. * CDHB / LambdaNP2
7796  +766821. * CDHW / LambdaNP2
7797  -4.054 * DeltaGF()
7798  ;
7799 
7800  // Add modifications due to small variations of the SM parameters
7801  mu += cHSM * ( -2.052 * deltaaMZ()
7802  +4.052 * deltaGmu()
7803  +8.704 * deltaMz()
7804  -0.351 * deltaMh() );
7805 
7806  } else {
7807  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7808  }
7809 
7810  } else if (sqrt_s == 1.0) {
7811 
7812  C1 = -0.0012;
7813 
7814  if (Pol_em == 80. && Pol_ep == -30.){
7815  mu +=
7816  +121236. * CHbox / LambdaNP2
7817  +2034785. * CHL1_11 / LambdaNP2
7818  -29195703. * CHe_11 / LambdaNP2
7819  +2034785. * CHL3_11 / LambdaNP2
7820  +74612.7 * CHD / LambdaNP2
7821  +1218284. * CHB / LambdaNP2
7822  +154779. * CHW / LambdaNP2
7823  +1507673. * CHWB / LambdaNP2
7824  +4701988. * CDHB / LambdaNP2
7825  +239404. * CDHW / LambdaNP2
7826  +0.458 * DeltaGF()
7827  ;
7828 
7829  // Add modifications due to small variations of the SM parameters
7830  mu += cHSM * ( +2.46 * deltaaMZ()
7831  -0.46 * deltaGmu()
7832  -0.745 * deltaMz()
7833  -0.092 * deltaMh() );
7834 
7835  } else if (Pol_em == -80. && Pol_ep == 30.){
7836  mu +=
7837  +121298. * CHbox / LambdaNP2
7838  +25954994. * CHL1_11 / LambdaNP2
7839  -1333713. * CHe_11 / LambdaNP2
7840  +25954994. * CHL3_11 / LambdaNP2
7841  -67536.7 * CHD / LambdaNP2
7842  -499699. * CHB / LambdaNP2
7843  +1872177. * CHW / LambdaNP2
7844  -263454. * CHWB / LambdaNP2
7845  -1999387. * CDHB / LambdaNP2
7846  +3910434. * CDHW / LambdaNP2
7847  -4.233 * DeltaGF()
7848  ;
7849 
7850  // Add modifications due to small variations of the SM parameters
7851  mu += cHSM * ( -2.23 * deltaaMZ()
7852  +4.23 * deltaGmu()
7853  +8.633 * deltaMz()
7854  -0.092 * deltaMh() );
7855 
7856  } else if (Pol_em == 80. && Pol_ep == 0.){
7857  mu +=
7858  +121307. * CHbox / LambdaNP2
7859  +3550656. * CHL1_11 / LambdaNP2
7860  -27432206. * CHe_11 / LambdaNP2
7861  +3550656. * CHL3_11 / LambdaNP2
7862  +65607.4 * CHD / LambdaNP2
7863  +1109435. * CHB / LambdaNP2
7864  +263679. * CHW / LambdaNP2
7865  +1395519. * CHWB / LambdaNP2
7866  +4277336. * CDHB / LambdaNP2
7867  +472106. * CDHW / LambdaNP2
7868  +0.159 * DeltaGF()
7869  ;
7870 
7871  // Add modifications due to small variations of the SM parameters
7872  mu += cHSM * ( +2.163 * deltaaMZ()
7873  -0.163 * deltaGmu()
7874  -0.151 * deltaMz()
7875  -0.092 * deltaMh() );
7876 
7877  } else if (Pol_em == -80. && Pol_ep == 0.){
7878  mu +=
7879  +121327. * CHbox / LambdaNP2
7880  +25048839. * CHL1_11 / LambdaNP2
7881  -2390358. * CHe_11 / LambdaNP2
7882  +25048839. * CHL3_11 / LambdaNP2
7883  -62132.7 * CHD / LambdaNP2
7884  -434824. * CHB / LambdaNP2
7885  +1807095. * CHW / LambdaNP2
7886  -196264. * CHWB / LambdaNP2
7887  -1746222. * CDHB / LambdaNP2
7888  +3771341. * CDHW / LambdaNP2
7889  -4.056 * DeltaGF()
7890  ;
7891 
7892  // Add modifications due to small variations of the SM parameters
7893  mu += cHSM * ( -2.052 * deltaaMZ()
7894  +4.052 * deltaGmu()
7895  +8.278 * deltaMz()
7896  -0.092 * deltaMh() );
7897 
7898  } else {
7899  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7900  }
7901 
7902  } else if (sqrt_s == 1.4) {
7903 
7904  C1 = -0.0011;
7905 
7906  if (Pol_em == 80. && Pol_ep == -30.){
7907  mu +=
7908  +121277. * CHbox / LambdaNP2
7909  +3988231. * CHL1_11 / LambdaNP2
7910  -57226150. * CHe_11 / LambdaNP2
7911  +3988231. * CHL3_11 / LambdaNP2
7912  +74608.5 * CHD / LambdaNP2
7913  +1256970. * CHB / LambdaNP2
7914  +155358. * CHW / LambdaNP2
7915  +1542655. * CHWB / LambdaNP2
7916  +9506894. * CDHB / LambdaNP2
7917  +553431. * CDHW / LambdaNP2
7918  +0.457 * DeltaGF()
7919  ;
7920 
7921  // Add modifications due to small variations of the SM parameters
7922  mu += cHSM * ( +2.46 * deltaaMZ()
7923  -0.46 * deltaGmu()
7924  -0.828 * deltaMz()
7925  -0.047 * deltaMh() );
7926 
7927  } else if (Pol_em == -80. && Pol_ep == 30.){
7928  mu +=
7929  +121314. * CHbox / LambdaNP2
7930  +50871646. * CHL1_11 / LambdaNP2
7931  -2614134. * CHe_11 / LambdaNP2
7932  +50871646. * CHL3_11 / LambdaNP2
7933  -67535.5 * CHD / LambdaNP2
7934  -516385. * CHB / LambdaNP2
7935  +1928805. * CHW / LambdaNP2
7936  -264072. * CHWB / LambdaNP2
7937  -3989947. * CDHB / LambdaNP2
7938  +7948308. * CDHW / LambdaNP2
7939  -4.233 * DeltaGF()
7940  ;
7941 
7942  // Add modifications due to small variations of the SM parameters
7943  mu += cHSM * ( -2.23 * deltaaMZ()
7944  +4.23 * deltaGmu()
7945  +8.55 * deltaMz()
7946  -0.047 * deltaMh() );
7947 
7948  } else if (Pol_em == 80. && Pol_ep == 0.){
7949  mu +=
7950  +121250. * CHbox / LambdaNP2
7951  +6958750. * CHL1_11 / LambdaNP2
7952  -53762500. * CHe_11 / LambdaNP2
7953  +6958750. * CHL3_11 / LambdaNP2
7954  +65589.3 * CHD / LambdaNP2
7955  +1144464. * CHB / LambdaNP2
7956  +267732. * CHW / LambdaNP2
7957  +1428214. * CHWB / LambdaNP2
7958  +8650536. * CDHB / LambdaNP2
7959  +1021964. * CDHW / LambdaNP2
7960  +0.16 * DeltaGF()
7961  ;
7962 
7963  // Add modifications due to small variations of the SM parameters
7964  mu += cHSM * ( +2.163 * deltaaMZ()
7965  -0.163 * deltaGmu()
7966  -0.234 * deltaMz()
7967  -0.047 * deltaMh() );
7968 
7969  } else if (Pol_em == -80. && Pol_ep == 0.){
7970  mu +=
7971  +121278. * CHbox / LambdaNP2
7972  +49094486. * CHL1_11 / LambdaNP2
7973  -4685522. * CHe_11 / LambdaNP2
7974  +49094486. * CHL3_11 / LambdaNP2
7975  -62150.9 * CHD / LambdaNP2
7976  -450090. * CHB / LambdaNP2
7977  +1861602. * CHW / LambdaNP2
7978  -195621. * CHWB / LambdaNP2
7979  -3478338. * CDHB / LambdaNP2
7980  +7668095. * CDHW / LambdaNP2
7981  -4.055 * DeltaGF()
7982  ;
7983 
7984  // Add modifications due to small variations of the SM parameters
7985  mu += cHSM * ( -2.052 * deltaaMZ()
7986  +4.052 * deltaGmu()
7987  +8.195 * deltaMz()
7988  -0.047 * deltaMh() );
7989 
7990  } else {
7991  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
7992  }
7993 
7994  } else if (sqrt_s == 1.5) {
7995 
7996  C1 = -0.0011;// Use the same as 1400 GeV
7997 
7998  if (Pol_em == 80. && Pol_ep == -30.){
7999  mu +=
8000  +121268. * CHbox / LambdaNP2
8001  +4578315. * CHL1_11 / LambdaNP2
8002  -65691823. * CHe_11 / LambdaNP2
8003  +4578315. * CHL3_11 / LambdaNP2
8004  +74595.2 * CHD / LambdaNP2
8005  +1262261. * CHB / LambdaNP2
8006  +155435. * CHW / LambdaNP2
8007  +1547379. * CHWB / LambdaNP2
8008  +10961322. * CDHB / LambdaNP2
8009  +649157. * CDHW / LambdaNP2
8010  +0.457 * DeltaGF()
8011  ;
8012 
8013  // Add modifications due to small variations of the SM parameters
8014  mu += cHSM * ( +2.46 * deltaaMZ()
8015  -0.46 * deltaGmu()
8016  -0.84 * deltaMz()
8017  -0.041 * deltaMh() );
8018 
8019  } else if (Pol_em == -80. && Pol_ep == 30.){
8020  mu +=
8021  +121277. * CHbox / LambdaNP2
8022  +58398883. * CHL1_11 / LambdaNP2
8023  -3000385. * CHe_11 / LambdaNP2
8024  +58398883. * CHL3_11 / LambdaNP2
8025  -67535.8 * CHD / LambdaNP2
8026  -518798. * CHB / LambdaNP2
8027  +1936613. * CHW / LambdaNP2
8028  -264171. * CHWB / LambdaNP2
8029  -4590136. * CDHB / LambdaNP2
8030  +9169803. * CDHW / LambdaNP2
8031  -4.233 * DeltaGF()
8032  ;
8033 
8034  // Add modifications due to small variations of the SM parameters
8035  mu += cHSM * ( -2.23 * deltaaMZ()
8036  +4.23 * deltaGmu()
8037  +8.539 * deltaMz()
8038  -0.041 * deltaMh() );
8039 
8040  } else if (Pol_em == 80. && Pol_ep == 0.){
8041  mu +=
8042  +121289. * CHbox / LambdaNP2
8043  +7988570. * CHL1_11 / LambdaNP2
8044  -61718691. * CHe_11 / LambdaNP2
8045  +7988570. * CHL3_11 / LambdaNP2
8046  +65599. * CHD / LambdaNP2
8047  +1149083. * CHB / LambdaNP2
8048  +268317. * CHW / LambdaNP2
8049  +1432777. * CHWB / LambdaNP2
8050  +9972576. * CDHB / LambdaNP2
8051  +1188554. * CDHW / LambdaNP2
8052  +0.16 * DeltaGF()
8053  ;
8054 
8055  // Add modifications due to small variations of the SM parameters
8056  mu += cHSM * ( +2.163 * deltaaMZ()
8057  -0.163 * deltaGmu()
8058  -0.246 * deltaMz()
8059  -0.041 * deltaMh() );
8060 
8061  } else if (Pol_em == -80. && Pol_ep == 0.){
8062  mu +=
8063  +121259. * CHbox / LambdaNP2
8064  +56356946. * CHL1_11 / LambdaNP2
8065  -5378233. * CHe_11 / LambdaNP2
8066  +56356946. * CHL3_11 / LambdaNP2
8067  -62168.7 * CHD / LambdaNP2
8068  -452149. * CHB / LambdaNP2
8069  +1869136. * CHW / LambdaNP2
8070  -195562. * CHWB / LambdaNP2
8071  -4000306. * CDHB / LambdaNP2
8072  +8846432. * CDHW / LambdaNP2
8073  -4.055 * DeltaGF()
8074  ;
8075 
8076  // Add modifications due to small variations of the SM parameters
8077  mu += cHSM * ( -2.052 * deltaaMZ()
8078  +4.052 * deltaGmu()
8079  +8.183 * deltaMz()
8080  -0.041 * deltaMh() );
8081 
8082  } else {
8083  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8084  }
8085 
8086  } else if (sqrt_s == 3.0) {
8087 
8088  C1 = -0.00054;
8089 
8090  if (Pol_em == 80. && Pol_ep == -30.){
8091  mu +=
8092  +121320. * CHbox / LambdaNP2
8093  +18314161. * CHL1_11 / LambdaNP2
8094  -262773345. * CHe_11 / LambdaNP2
8095  +18314161. * CHL3_11 / LambdaNP2
8096  +74663.6 * CHD / LambdaNP2
8097  +1289569. * CHB / LambdaNP2
8098  +155612. * CHW / LambdaNP2
8099  +1572580. * CHWB / LambdaNP2
8100  +44806408. * CDHB / LambdaNP2
8101  +2877519. * CDHW / LambdaNP2
8102  +0.456 * DeltaGF()
8103  ;
8104 
8105  // Add modifications due to small variations of the SM parameters
8106  mu += cHSM * ( +2.46 * deltaaMZ()
8107  -0.46 * deltaGmu()
8108  -0.899 * deltaMz()
8109  -0.01 * deltaMh() );
8110 
8111  } else if (Pol_em == -80. && Pol_ep == 30.){
8112  mu +=
8113  +121305. * CHbox / LambdaNP2
8114  +233598342. * CHL1_11 / LambdaNP2
8115  -12002450. * CHe_11 / LambdaNP2
8116  +233598342. * CHL3_11 / LambdaNP2
8117  -67507.7 * CHD / LambdaNP2
8118  -531387. * CHB / LambdaNP2
8119  +1976750. * CHW / LambdaNP2
8120  -264661. * CHWB / LambdaNP2
8121  -18587969. * CDHB / LambdaNP2
8122  +37618569. * CDHW / LambdaNP2
8123  -4.233 * DeltaGF()
8124  ;
8125 
8126  // Add modifications due to small variations of the SM parameters
8127  mu += cHSM * ( -2.23 * deltaaMZ()
8128  +4.23 * deltaGmu()
8129  +8.48 * deltaMz()
8130  -0.01 * deltaMh() );
8131 
8132  } else if (Pol_em == 80. && Pol_ep == 0.){
8133  mu +=
8134  +121225. * CHbox / LambdaNP2
8135  +31953446. * CHL1_11 / LambdaNP2
8136  -246870182. * CHe_11 / LambdaNP2
8137  +31953446. * CHL3_11 / LambdaNP2
8138  +65576.5 * CHD / LambdaNP2
8139  +1173703. * CHB / LambdaNP2
8140  +270983. * CHW / LambdaNP2
8141  +1456032. * CHWB / LambdaNP2
8142  +40783748. * CDHB / LambdaNP2
8143  +5077924. * CDHW / LambdaNP2
8144  +0.16 * DeltaGF()
8145  ;
8146 
8147  // Add modifications due to small variations of the SM parameters
8148  mu += cHSM * ( +2.163 * deltaaMZ()
8149  -0.163 * deltaGmu()
8150  -0.305 * deltaMz()
8151  -0.01 * deltaMh() );
8152 
8153  } else if (Pol_em == -80. && Pol_ep == 0.){
8154  mu +=
8155  +121248. * CHbox / LambdaNP2
8156  +225427310. * CHL1_11 / LambdaNP2
8157  -21505526. * CHe_11 / LambdaNP2
8158  +225427310. * CHL3_11 / LambdaNP2
8159  -62193.4 * CHD / LambdaNP2
8160  -463403. * CHB / LambdaNP2
8161  +1907593. * CHW / LambdaNP2
8162  -195017. * CHWB / LambdaNP2
8163  -16188019. * CDHB / LambdaNP2
8164  +36299719. * CDHW / LambdaNP2
8165  -4.054 * DeltaGF()
8166  ;
8167 
8168  // Add modifications due to small variations of the SM parameters
8169  mu += cHSM * ( -2.052 * deltaaMZ()
8170  +4.052 * deltaGmu()
8171  +8.124 * deltaMz()
8172  -0.01 * deltaMh() );
8173 
8174  } else {
8175  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8176  }
8177 
8178  } else
8179  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8180 
8181  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8182  mu += eeeZHint + eeeZHpar;
8183 
8184 // Linear contribution from Higgs self-coupling
8185  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8186 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8188 
8189  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8190 
8191  return mu;
8192 }
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3649
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3648
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref...
Definition: NPSMEFTd6.cpp:2465
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:2454
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2399
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2388

◆ mueeZllH()

double NPSMEFTd6::mueeZllH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 7207 of file NPSMEFTd6.cpp.

7208 {
7209 
7210 // The signal strength eeZH
7211  double mu = mueeZH(sqrt_s);
7212 
7213 // The (relative) linear correction to the Z>ll BR
7214  double deltaBRratio;
7215 
7216  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
7217  + deltaGamma_Zf(leptons[MU]);
7218 
7219  deltaBRratio = deltaBRratio /
7221 
7222  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7223 
7224  return mu + deltaBRratio;
7225 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: QCD.h:605
virtual double mueeZH(const double sqrt_s) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:6895

◆ mueeZllHPol()

double NPSMEFTd6::mueeZllHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 8194 of file NPSMEFTd6.cpp.

8195 {
8196 
8197 // The signal strength eeZH
8198  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8199 
8200 // The (relative) linear correction to the Z>ll BR
8201  double deltaBRratio;
8202 
8203  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
8204  + deltaGamma_Zf(leptons[MU]);
8205 
8206  deltaBRratio = deltaBRratio /
8208 
8209  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8210 
8211  return mu + deltaBRratio;
8212 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double mueeZHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7252
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: QCD.h:605

◆ mueeZqqH()

double NPSMEFTd6::mueeZqqH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 7227 of file NPSMEFTd6.cpp.

7228 {
7229 
7230 // The signal strength eeZH
7231  double mu = mueeZH(sqrt_s);
7232 
7233 // The (relative) linear correction to the Z>qq BR
7234  double deltaBRratio;
7235 
7236  deltaBRratio = deltaGamma_Zf(quarks[UP])
7241 
7242  deltaBRratio = deltaBRratio /
7245  + trueSM.GammaZ(quarks[BOTTOM]));
7246 
7247  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7248 
7249  return mu + deltaBRratio;
7250 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
Definition: QCD.h:615
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Definition: QCD.h:616
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual double mueeZH(const double sqrt_s) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:6895

◆ mueeZqqHPol()

double NPSMEFTd6::mueeZqqHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 8214 of file NPSMEFTd6.cpp.

8215 {
8216 
8217 // The signal strength eeZH
8218  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8219 
8220 // The (relative) linear correction to the Z>qq BR
8221  double deltaBRratio;
8222 
8223  deltaBRratio = deltaGamma_Zf(quarks[UP])
8228 
8229  deltaBRratio = deltaBRratio /
8232  + trueSM.GammaZ(quarks[BOTTOM]));
8233 
8234  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8235 
8236  return mu + deltaBRratio;
8237 }
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair...
Definition: NPbase.cpp:135
StandardModel trueSM
Definition: NPbase.h:1902
virtual double mueeZHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7252
Definition: QCD.h:615
virtual double Gamma_Z() const
The total decay width of the boson, .
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
virtual double GammaZ(const Particle f) const
The partial decay width, .
Definition: QCD.h:616
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222

◆ muepWBF()

double NPSMEFTd6::muepWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epWBF}\)

Reimplemented from NPbase.

Definition at line 6330 of file NPSMEFTd6.cpp.

6331 {
6332  double mu = 1.0;
6333 
6334  if (sqrt_s == 1.3) {
6335 
6336  mu +=
6337  +121790. * CHbox / LambdaNP2
6338  -161604. * CHL3_11 / LambdaNP2
6339  -161282. * CHQ3_11 / LambdaNP2
6340  -203141. * CHD / LambdaNP2
6341  -88171.6 * CHW / LambdaNP2
6342  -377218. * CHWB / LambdaNP2
6343  -37738.9 * CDHW / LambdaNP2
6344  -4.676 * DeltaGF()
6345  -4.916 * deltaMwd6()
6346  ;
6347 
6348 // if (FlagQuadraticTerms) {
6349  //Add contributions that are quadratic in the effective coefficients
6350 
6351 // }
6352 
6353  } else if (sqrt_s == 1.8) {
6354 
6355  mu +=
6356  +121867. * CHbox / LambdaNP2
6357  -182643. * CHL3_11 / LambdaNP2
6358  -181961. * CHQ3_11 / LambdaNP2
6359  -202400. * CHD / LambdaNP2
6360  -78295.8 * CHW / LambdaNP2
6361  -377193. * CHWB / LambdaNP2
6362  -45757.3 * CDHW / LambdaNP2
6363  -4.672 * DeltaGF()
6364  -4.637 * deltaMwd6()
6365  ;
6366 
6367 // if (FlagQuadraticTerms) {
6368  //Add contributions that are quadratic in the effective coefficients
6369 
6370 // }
6371 
6372  } else if (sqrt_s == 3.5) {
6373 
6374  mu +=
6375  +121250. * CHbox / LambdaNP2
6376  -216885. * CHL3_11 / LambdaNP2
6377  -218544. * CHQ3_11 / LambdaNP2
6378  -202390. * CHD / LambdaNP2
6379  -64783.2 * CHW / LambdaNP2
6380  -377727. * CHWB / LambdaNP2
6381  -60431.2 * CDHW / LambdaNP2
6382  -4.688 * DeltaGF()
6383  -4.573 * deltaMwd6()
6384  ;
6385 
6386 // if (FlagQuadraticTerms) {
6387  //Add contributions that are quadratic in the effective coefficients
6388 
6389 // }
6390 
6391  } else if (sqrt_s == 5.0) {
6392 
6393  mu +=
6394  +119662. * CHbox / LambdaNP2
6395  -237868. * CHL3_11 / LambdaNP2
6396  -236470. * CHQ3_11 / LambdaNP2
6397  -203294. * CHD / LambdaNP2
6398  -60911. * CHW / LambdaNP2
6399  -378045. * CHWB / LambdaNP2
6400  -67483.7 * CDHW / LambdaNP2
6401  -4.667 * DeltaGF()
6402  -4.437 * deltaMwd6()
6403  ;
6404 
6405 // if (FlagQuadraticTerms) {
6406  //Add contributions that are quadratic in the effective coefficients
6407 
6408 // }
6409 
6410  } else
6411  throw std::runtime_error("Bad argument in NPSMEFTd6::muepWBF()");
6412 
6413  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6414 
6415  return mu;
6416 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439

◆ muepZBF()

double NPSMEFTd6::muepZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epZBF}\)

Reimplemented from NPbase.

Definition at line 6418 of file NPSMEFTd6.cpp.

6419 {
6420  double mu = 1.0;
6421 
6422  if (sqrt_s == 1.3) {
6423 
6424  mu +=
6425  +121280. * CHbox / LambdaNP2
6426  -152367. * CHL1_11 / LambdaNP2
6427  +32200. * CHQ1_11 / LambdaNP2
6428  +124934. * CHe_11 / LambdaNP2
6429  -42209.5 * CHu_11 / LambdaNP2
6430  +12445.7 * CHd_11 / LambdaNP2
6431  -152367. * CHL3_11 / LambdaNP2
6432  -165343. * CHQ3_11 / LambdaNP2
6433  -173922. * CHD / LambdaNP2
6434  -34636.2 * CHB / LambdaNP2
6435  -121438. * CHW / LambdaNP2
6436  -74939.1 * CHWB / LambdaNP2
6437  -5454.93 * CDHB / LambdaNP2
6438  -39349.6 * CDHW / LambdaNP2
6439  -3.719 * DeltaGF()
6440  ;
6441 
6442 // if (FlagQuadraticTerms) {
6443  //Add contributions that are quadratic in the effective coefficients
6444 
6445 // }
6446 
6447  } else if (sqrt_s == 1.8) {
6448 
6449  mu +=
6450  +120218. * CHbox / LambdaNP2
6451  -173566. * CHL1_11 / LambdaNP2
6452  +26307.1 * CHQ1_11 / LambdaNP2
6453  +142600. * CHe_11 / LambdaNP2
6454  -47449. * CHu_11 / LambdaNP2
6455  +14356.2 * CHd_11 / LambdaNP2
6456  -173566. * CHL3_11 / LambdaNP2
6457  -188606. * CHQ3_11 / LambdaNP2
6458  -174301. * CHD / LambdaNP2
6459  -19800. * CHB / LambdaNP2
6460  -103254. * CHW / LambdaNP2
6461  -89049.2 * CHWB / LambdaNP2
6462  -8304.85 * CDHB / LambdaNP2
6463  -48942.9 * CDHW / LambdaNP2
6464  -3.714 * DeltaGF()
6465  ;
6466 
6467 // if (FlagQuadraticTerms) {
6468  //Add contributions that are quadratic in the effective coefficients
6469 
6470 // }
6471 
6472  } else if (sqrt_s == 3.5) {
6473 
6474  mu +=
6475  +123119. * CHbox / LambdaNP2
6476  -206981. * CHL1_11 / LambdaNP2
6477  +18620.9 * CHQ1_11 / LambdaNP2
6478  +177706. * CHe_11 / LambdaNP2
6479  -53822. * CHu_11 / LambdaNP2
6480  +20491.5 * CHd_11 / LambdaNP2
6481  -206981. * CHL3_11 / LambdaNP2
6482  -227549. * CHQ3_11 / LambdaNP2
6483  -172298. * CHD / LambdaNP2
6484  -6887.17 * CHB / LambdaNP2
6485  -79245. * CHW / LambdaNP2
6486  -103223. * CHWB / LambdaNP2
6487  -9863.11 * CDHB / LambdaNP2
6488  -61304.3 * CDHW / LambdaNP2
6489  -3.721 * DeltaGF()
6490  ;
6491 
6492 // if (FlagQuadraticTerms) {
6493  //Add contributions that are quadratic in the effective coefficients
6494 
6495 // }
6496 
6497  } else if (sqrt_s == 5.0) {
6498 
6499  mu +=
6500  +121709. * CHbox / LambdaNP2
6501  -225267. * CHL1_11 / LambdaNP2
6502  +13471.8 * CHQ1_11 / LambdaNP2
6503  +193542. * CHe_11 / LambdaNP2
6504  -57640.9 * CHu_11 / LambdaNP2
6505  +22573. * CHd_11 / LambdaNP2
6506  -225267. * CHL3_11 / LambdaNP2
6507  -247738. * CHQ3_11 / LambdaNP2
6508  -172768. * CHD / LambdaNP2
6509  -4524.89 * CHB / LambdaNP2
6510  -71935.4 * CHW / LambdaNP2
6511  -104998. * CHWB / LambdaNP2
6512  -11877.8 * CDHB / LambdaNP2
6513  -69467.3 * CDHW / LambdaNP2
6514  -3.71 * DeltaGF()
6515  ;
6516 
6517 // if (FlagQuadraticTerms) {
6518  //Add contributions that are quadratic in the effective coefficients
6519 
6520 // }
6521 
6522  } else
6523  throw std::runtime_error("Bad argument in NPSMEFTd6::muepZBF()");
6524 
6525  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6526 
6527  return mu;
6528 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471

◆ muggH()

double NPSMEFTd6::muggH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH}\)

Reimplemented from NPbase.

Definition at line 3057 of file NPSMEFTd6.cpp.

3058 {
3059 
3060  double C1 = 0.0066; //It seems to be independent of energy
3061 
3062  double m_t = mtpole;
3063  //doulbe m_t = quarks[TOP].getMass();
3064  double m_b = quarks[BOTTOM].getMass();
3065  double m_c = quarks[CHARM].getMass();
3066 
3067  /* L_eff_SM = (G_eff_t_SM + G_eff_b_SM)*hGG */
3068  gslpp::complex G_eff_t_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_t * m_t / mHl / mHl);
3069  gslpp::complex G_eff_b_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_b * m_b / mHl / mHl);
3070  gslpp::complex G_eff_c_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_c * m_c / mHl / mHl);
3071  gslpp::complex G_eff_SM = G_eff_t_SM + G_eff_b_SM + G_eff_c_SM;
3072 
3073  //double sigma_tt_SM = trueSM.computeSigmaggH_tt(sqrt_s);
3074  //double sigma_bb_SM = trueSM.computeSigmaggH_bb(sqrt_s);
3075  //double sigma_tb_SM = trueSM.computeSigmaggH_tb(sqrt_s);
3076  //gslpp::complex tmp = (2.0 * dKappa_t * sigma_tt_SM
3077  // + 2.0 * dKappa_b * sigma_bb_SM
3078  // + (dKappa_t + dKappa_b) * sigma_tb_SM)
3079  // / (sigma_tt_SM + sigma_bb_SM + sigma_tb_SM);
3080 
3081  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3082  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3083  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3084 
3085  gslpp::complex tmpHG = CHG / v() * v2_over_LambdaNP2 / G_eff_SM;
3086  gslpp::complex tmpt = G_eff_t_SM * dKappa_t / G_eff_SM;
3087  gslpp::complex tmpb = G_eff_b_SM * dKappa_b / G_eff_SM;
3088  gslpp::complex tmpc = G_eff_c_SM * dKappa_c / G_eff_SM;
3089 
3090  double mu = (1.0 + 2.0 * ( tmpt.real() + tmpb.real() + tmpc.real() + tmpHG.real() ) );
3091 
3092 // Linear contribution from Higgs self-coupling
3093  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3094 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3096 
3097  if (FlagQuadraticTerms) {
3098  //Add contributions that are quadratic in the effective coefficients
3099  gslpp::complex tmp2 = tmpt +tmpb +tmpc + tmpHG;
3100 
3101  mu += tmp2.abs2();
3102 
3103  }
3104 
3105  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3106  mu += eggFint + eggFpar;
3107 
3108  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3109 
3110  return mu;
3111 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
const double & real() const
double eggFpar
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3637
double abs2() const
double AlsMz
The strong coupling constant at the Z-boson mass, .
double mHl
The Higgs mass in GeV.
Definition: QCD.h:619
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3029
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double eggFint
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3636
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ muggHbb()

double NPSMEFTd6::muggHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,bb}\)

Reimplemented from NPbase.

Definition at line 12152 of file NPSMEFTd6.cpp.

12153 {
12154  return muggH(sqrt_s) * BrHbbRatio();
12155 
12156 }
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHgaga()

double NPSMEFTd6::muggHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11864 of file NPSMEFTd6.cpp.

11865 {
11866  return muggH(sqrt_s) * BrHgagaRatio();
11867 
11868 }
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHH()

double NPSMEFTd6::muggHH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggHH}\)

Reimplemented from NPbase.

Definition at line 3113 of file NPSMEFTd6.cpp.

3114 {
3115  double mu = 1.0;
3116  double A1HH = 0.0, A2HH = 0.0, A3HH = 0.0, A4HH = 0.0, A5HH = 0.0;
3117  double A6HH = 0.0, A7HH = 0.0, A8HH = 0.0, A9HH = 0.0, A10HH = 0.0;
3118  double A11HH = 0.0, A12HH = 0.0, A13HH = 0.0, A14HH = 0.0, A15HH = 0.0;
3119  double ct,c2t,c3,cg,c2g;
3120 
3121  if (sqrt_s == 14.0) {
3122 
3123  // From the cut-based analysis. Table IV
3124 
3125  A1HH = 1.70;
3126  A2HH = 10.7;
3127  A3HH = 0.117;
3128  A4HH = 6.11;
3129  A5HH = 217.0;
3130  A6HH = -7.56;
3131  A7HH = -0.819;
3132  A8HH = 1.95;
3133  A9HH = 10.90;
3134  A10HH = 51.6;
3135  A11HH = -3.86;
3136  A12HH = -12.5;
3137  A13HH = 1.46;
3138  A14HH = 5.49;
3139  A15HH = 58.4;
3140 
3141  } else if (sqrt_s == 100.0) {
3142 
3143  // From the cut-based analysis. Table IV
3144 
3145  A1HH = 1.59;
3146  A2HH = 12.8;
3147  A3HH = 0.090;
3148  A4HH = 5.2;
3149  A5HH = 358.0;
3150  A6HH = -7.66;
3151  A7HH = -0.681;
3152  A8HH = 1.83;
3153  A9HH = 9.25;
3154  A10HH = 51.2;
3155  A11HH = -2.61;
3156  A12HH = -7.35;
3157  A13HH = 1.03;
3158  A14HH = 4.65;
3159  A15HH = 65.5;
3160 
3161  } else
3162  throw std::runtime_error("Bad argument in NPSMEFTd6::muggHH()");
3163 
3164  ct= 1.0 - 0.5 * DeltaGF() + delta_h - v() * CuH_33r * v2_over_LambdaNP2 / sqrt(2.0)/ mtpole;
3165  c2t = delta_h - 3.0 *v() * CuH_33r * v2_over_LambdaNP2 / 2.0 /sqrt(2.0)/ mtpole;
3166  c3 = 1.0 + deltaG_hhhRatio();
3167  cg = M_PI * CHG * v2_over_LambdaNP2 / AlsMz;
3168  c2g = cg;
3169 
3170 // In the SM the Eq. returns 0.999. Fix that small offset by adding 0.0010
3171  mu = 0.0010 + A1HH*ct*ct*ct*ct +
3172  A2HH*c2t*c2t +
3173  A3HH*ct*ct*c3*c3 +
3174  A4HH*cg*cg*c3*c3 +
3175  A5HH*c2g*c2g +
3176  A6HH*c2t*ct*ct +
3177  A7HH*ct*ct*ct*c3 +
3178  A8HH*c2t*ct*c3 +
3179  A9HH*c2t*cg*c3 +
3180  A10HH*c2t*c2g +
3181  A11HH*ct*ct*cg*c3 +
3182  A12HH*ct*ct*c2g +
3183  A13HH*ct*c3*c3*cg +
3184  A14HH*ct*c3*c2g +
3185  A15HH*cg*c3*c2g;
3186 
3187  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3188 
3189  return mu;
3190 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
double AlsMz
The strong coupling constant at the Z-boson mass, .
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
complex sqrt(const complex &z)

◆ muggHmumu()

double NPSMEFTd6::muggHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12080 of file NPSMEFTd6.cpp.

12081 {
12082  return muggH(sqrt_s) * BrHmumuRatio();
12083 
12084 }
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHpttH()

double NPSMEFTd6::muggHpttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH+ttH}\)

Reimplemented from NPbase.

Definition at line 8408 of file NPSMEFTd6.cpp.

8409 {
8410  double sigmaggH_SM = computeSigmaggH(sqrt_s);
8411  double sigmattH_SM = computeSigmattH(sqrt_s);
8412  double sigmaggH = muggH(sqrt_s) * sigmaggH_SM;
8413  double sigmattH = muttH(sqrt_s) * sigmattH_SM;
8414 
8415  double mu = ((sigmaggH + sigmattH) / (sigmaggH_SM + sigmattH_SM));
8416 
8417  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8418 
8419  return mu;
8420 }
double computeSigmaggH(const double sqrt_s) const
The ggH cross section in the Standard Model.
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057
double computeSigmattH(const double sqrt_s) const
The ttH production cross section in the Standard Model.

◆ muggHtautau()

double NPSMEFTd6::muggHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12116 of file NPSMEFTd6.cpp.

12117 {
12118  return muggH(sqrt_s) * BrHtautauRatio();
12119 
12120 }
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHWW()

double NPSMEFTd6::muggHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW}\)

Reimplemented from NPbase.

Definition at line 12008 of file NPSMEFTd6.cpp.

12009 {
12010  return muggH(sqrt_s) * BrHWWRatio();
12011 
12012 }
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muggHWW2l2v()

double NPSMEFTd6::muggHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12044 of file NPSMEFTd6.cpp.

12045 {
12046  return muggH(sqrt_s) * BrHWW2l2vRatio();
12047 
12048 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHZga()

double NPSMEFTd6::muggHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11900 of file NPSMEFTd6.cpp.

11901 {
11902  return muggH(sqrt_s) * BrHZgaRatio();
11903 
11904 }
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHZZ()

double NPSMEFTd6::muggHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ}\)

Reimplemented from NPbase.

Definition at line 11936 of file NPSMEFTd6.cpp.

11937 {
11938  return muggH(sqrt_s) * BrHZZRatio();
11939 
11940 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057

◆ muggHZZ4l()

double NPSMEFTd6::muggHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 11972 of file NPSMEFTd6.cpp.

11973 {
11974  return muggH(sqrt_s) * BrHZZ4lRatio();
11975 
11976 }
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3057
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ mummH()

double NPSMEFTd6::mummH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{\mu\mu H}\)

Reimplemented from NPbase.

Definition at line 9221 of file NPSMEFTd6.cpp.

9222 {
9223  double mu = 1.0;
9224 
9225  double dymu = deltaG_hff(leptons[MU]).real();
9226  double ymuSM = -(leptons[MU].getMass()) / v();
9227 
9228 // The ratio at all energies is given by a scaling of the muon Yukawa.
9229  mu = 1.0 + 2.0 * dymu/ymuSM ;
9230 
9231  if (FlagQuadraticTerms) {
9232  //Add contributions that are quadratic in the effective coefficients
9233  mu += dymu*dymu/ymuSM/ymuSM;
9234  }
9235 
9236  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9237 
9238  return mu;
9239 }
const double & real() const
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
Particle leptons[6]
An array of Particle objects for the leptons.
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
Definition: QCD.h:605

◆ mupTVppWZ()

double NPSMEFTd6::mupTVppWZ ( const double  sqrt_s,
const double  pTV1,
const double  pTV2 
) const
virtual

The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.

Returns
\(N_{ev}^{p_{TV}}/N_{ev,SM}^{p_{TV}}\)

Reimplemented from NPbase.

Definition at line 12623 of file NPSMEFTd6.cpp.

12624 {
12625  double mu = 1.0;
12626 
12627  double cHWp = 0.0;
12628 
12629  // In the Warsaw basis the contact interactions are generated only by CHQ3 but
12630  // in the modified basis ODHW also contribute
12631 
12632  cHWp = (sW2_tree/eeMz2) * (CHQ3_11 + (g2_tree/4.0) * CDHW) / LambdaNP2;
12633 
12634 // Bin dependences assuming cutoff of the EFT at 5 TeV
12635 // Normalize to the total number of events to remove the dependence on Lumi
12636 // (Numbers correspond to 3/ab)
12637  if (sqrt_s == 14.0) {
12638 
12639  if (pTV1 == 100.){
12640  mu += (558.0 * cHWp + 56.8 * cHWp * cHWp) / 3450.0;
12641 
12642  } else if (pTV1 == 150.){
12643  mu += (410.0 * cHWp + 17.64 * cHWp * cHWp) / 2690.0;
12644 
12645  } else if (pTV1 == 220.){
12646  mu += (266.0 * cHWp + 45.6 * cHWp * cHWp) / 925.0;
12647 
12648  } else if (pTV1 == 300.){
12649  mu += (304.0 * cHWp + 108.0 * cHWp * cHWp) / 563.0;
12650 
12651  } else if (pTV1 == 500.){
12652  mu += (114.40 * cHWp + 96.8 * cHWp * cHWp) / 85.1 ;
12653 
12654  } else if (pTV1 == 750.){
12655  mu += (46.20 * cHWp + 86.8 * cHWp * cHWp) / 14.9;
12656 
12657  } else {
12658  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
12659  }
12660 
12661  } else if (sqrt_s == 27.0) {
12662 
12663  if (pTV1 == 150.){
12664  mu += (824.0 * cHWp + 71.6 * cHWp * cHWp) / 5370.0;
12665 
12666  } else if (pTV1 == 220.){
12667  mu += (510.0 * cHWp + 75.2 * cHWp * cHWp) / 2210.0;
12668 
12669  } else if (pTV1 == 300.){
12670  mu += (808.0 * cHWp + 268.4 * cHWp * cHWp) / 1610.0;
12671 
12672  } else if (pTV1 == 500.){
12673  mu += (374.0 * cHWp + 308.0 * cHWp * cHWp) / 331.0;
12674 
12675  } else if (pTV1 == 750.){
12676  mu += (216.0 * cHWp + 420.0 * cHWp * cHWp) / 85.9;
12677 
12678  } else if (pTV1 == 1200.){
12679  mu += (78.2 * cHWp + 325.2 * cHWp * cHWp) / 10.0;
12680 
12681  } else {
12682  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
12683  }
12684 
12685  } else if (sqrt_s == 100.0) {
12686 
12687  if (pTV1 == 220.){
12688  mu += (2000.0 * cHWp + 368.4 * cHWp * cHWp) / 8030.0;
12689 
12690  } else if (pTV1 == 300.){
12691  mu += (2780.0 * cHWp + 1000.0 * cHWp * cHWp) / 7270.0;
12692 
12693  } else if (pTV1 == 500.){
12694  mu += (1544.0 * cHWp + 1428.0 * cHWp * cHWp) / 2000.0;
12695 
12696  } else if (pTV1 == 750.){
12697  mu += (1256.0 * cHWp + 2668.0 * cHWp * cHWp) / 717.0;
12698 
12699  } else if (pTV1 == 1200.){
12700  mu += (678.0 * cHWp + 3400.0 * cHWp * cHWp) / 142.0;
12701 
12702  } else if (pTV1 == 1800.){
12703  mu += (234.0 * cHWp + 2540.0 * cHWp * cHWp) / 27.5;
12704 
12705  } else {
12706  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
12707  }
12708 
12709  } else
12710  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
12711 
12712  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
12713 
12714  return mu;
12715 
12716 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3811
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804

◆ muttH()

double NPSMEFTd6::muttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH}\)

Reimplemented from NPbase.

Definition at line 8267 of file NPSMEFTd6.cpp.

8268 {
8269  double mu = 1.0;
8270 
8271  double C1 = 0.0;
8272 
8273  if (sqrt_s == 1.96) {
8274 
8275  C1 = 0.0; // N.A.
8276 
8277  mu +=
8278  +423420. * (1. + ettH_2_HG ) * CHG / LambdaNP2
8279  -4269.4 * (1. + ettH_2_G ) * CG / LambdaNP2
8280  +566792. * (1. + ettH_2_uG_33r ) * CuG_33r / LambdaNP2
8281  -2.854 * (1. + ettH_2_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8282  ;
8283 
8284  if (FlagQuadraticTerms) {
8285  //Add contributions that are quadratic in the effective coefficients
8286  mu += 0.0;
8287 
8288  }
8289 
8290  } else if (sqrt_s == 7.0) {
8291 
8292  C1 = 0.0387;
8293 
8294  mu +=
8295  +532200. * (1. + ettH_78_HG ) * CHG / LambdaNP2
8296  -85145.2 * (1. + ettH_78_G ) * CG / LambdaNP2
8297  +811678. * (1. + ettH_78_uG_33r ) * CuG_33r / LambdaNP2
8298  -2.841 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8299  ;
8300 
8301  if (FlagQuadraticTerms) {
8302  //Add contributions that are quadratic in the effective coefficients
8303  mu += 0.0;
8304 
8305  }
8306 
8307  } else if (sqrt_s == 8.0) {
8308 
8309  C1 = 0.0378;
8310 
8311  mu +=
8312  +535632. * (1. + ettH_78_HG ) * CHG / LambdaNP2
8313  -86537.2 * (1. + ettH_78_G ) * CG / LambdaNP2
8314  +825379. * (1. + ettH_78_uG_33r ) * CuG_33r / LambdaNP2
8315  -2.849 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8316  ;
8317 
8318  if (FlagQuadraticTerms) {
8319  //Add contributions that are quadratic in the effective coefficients
8320  mu += 0.0;
8321 
8322  }
8323 
8324  } else if (sqrt_s == 13.0) {
8325 
8326  C1 = 0.0351;
8327 
8328  mu +=
8329  +538764. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
8330  -84648. * (1. + ettH_1314_G ) * CG / LambdaNP2
8331  +860470. * (1. + ettH_1314_uG_33r ) * CuG_33r / LambdaNP2
8332  -2.834 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8333  ;
8334 
8335  if (FlagQuadraticTerms) {
8336  //Add contributions that are quadratic in the effective coefficients
8337  mu += 0.0;
8338 
8339  }
8340 
8341  } else if (sqrt_s == 14.0) {
8342 
8343  C1 = 0.0347;
8344 
8345  mu +=
8346  +536600. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
8347  -83824.6 * (1. + ettH_1314_G ) * CG / LambdaNP2
8348  +863670. * (1. + ettH_1314_uG_33r ) * CuG_33r / LambdaNP2
8349  -2.839 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
8350  ;
8351 
8352  if (FlagQuadraticTerms) {
8353  //Add contributions that are quadratic in the effective coefficients
8354  mu += 0.0;
8355 
8356  }
8357 
8358  } else if (sqrt_s == 27.0) {
8359 
8360  C1 = 0.0; // N.A.
8361 
8362  mu +=
8363  +519682. * CHG / LambdaNP2
8364  -68463.1 * CG / LambdaNP2
8365  +884060. * CuG_33r / LambdaNP2
8366  -2.849 * deltaG_hff(quarks[TOP]).real()
8367  ;
8368 
8369  if (FlagQuadraticTerms) {
8370  //Add contributions that are quadratic in the effective coefficients
8371  mu += 0.0;
8372 
8373  }
8374 
8375  } else if (sqrt_s == 100.0) {
8376 
8377  C1 = 0.0; // N.A.
8378 
8379  mu +=
8380  +467438. * CHG / LambdaNP2
8381  -22519. * CG / LambdaNP2
8382  +880378. * CuG_33r / LambdaNP2
8383  -2.837 * deltaG_hff(quarks[TOP]).real()
8384  ;
8385 
8386  if (FlagQuadraticTerms) {
8387  //Add contributions that are quadratic in the effective coefficients
8388  mu += 0.0;
8389 
8390  }
8391 
8392  } else
8393  throw std::runtime_error("Bad argument in NPSMEFTd6::muttH()");
8394 
8395  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8396  mu += ettHint + ettHpar;
8397 
8398 // Linear contribution from Higgs self-coupling
8399  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8400 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8402 
8403  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8404 
8405  return mu;
8406 }
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3429
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
const double & real() const
double ettH_2_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3778
double ettHpar
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3639
double ettH_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3776
double ettH_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3781
Definition: QCD.h:619
double ettH_1314_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3787
double ettH_2_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3777
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double ettH_1314_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3788
double ettH_78_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3784
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double ettH_78_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3783
double ettH_2_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3779
double ettH_78_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3782
double ettH_1314_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3789
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double ettH_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3786
double ettHint
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3638
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ muttHbb()

double NPSMEFTd6::muttHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,bb}\)

Reimplemented from NPbase.

Definition at line 12182 of file NPSMEFTd6.cpp.

12183 {
12184  return muttH(sqrt_s) * BrHbbRatio();
12185 
12186 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905

◆ muttHgaga()

double NPSMEFTd6::muttHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11894 of file NPSMEFTd6.cpp.

11895 {
11896  return muttH(sqrt_s) * BrHgagaRatio();
11897 
11898 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801

◆ muttHmumu()

double NPSMEFTd6::muttHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12110 of file NPSMEFTd6.cpp.

12111 {
12112  return muttH(sqrt_s) * BrHmumuRatio();
12113 
12114 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827

◆ muttHtautau()

double NPSMEFTd6::muttHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12146 of file NPSMEFTd6.cpp.

12147 {
12148  return muttH(sqrt_s) * BrHtautauRatio();
12149 
12150 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853

◆ muttHWW()

double NPSMEFTd6::muttHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW}\)

Reimplemented from NPbase.

Definition at line 12038 of file NPSMEFTd6.cpp.

12039 {
12040  return muttH(sqrt_s) * BrHWWRatio();
12041 
12042 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muttHWW2l2v()

double NPSMEFTd6::muttHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12074 of file NPSMEFTd6.cpp.

12075 {
12076  return muttH(sqrt_s) * BrHWW2l2vRatio();
12077 
12078 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267

◆ muttHZbbboost()

double NPSMEFTd6::muttHZbbboost ( const double  sqrt_s) const
virtual

The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\sigma(ttH)/\sigma(ttZ)\) normalized to the SM

Reimplemented from NPbase.

Definition at line 11808 of file NPSMEFTd6.cpp.

11809 {
11810  /* Ratios of BR with the SM*/
11811  double BrHbbrat = BrHbbRatio();
11812  double BrZbbSM = (trueSM.GammaZ(quarks[BOTTOM]))/trueSM.Gamma_Z();
11813  double BrZbbrat = BR_Zf(quarks[BOTTOM])/BrZbbSM;
11814 
11815 // gslpp::complex dKappa_t = deltaG_hff(quarks[TOP]) / (-mtpole / v());
11816 // double dkt = dKappa_t.real();
11817 
11818 // double dgV = deltaGV_f(quarks[TOP]);
11819 // double dgA = deltaGA_f(quarks[TOP]);
11820 // double gLSM = quarks[TOP].getIsospin()
11821 // - (quarks[TOP].getCharge())*sW2_tree;
11822 // double gRSM = - (quarks[TOP].getCharge())*sW2_tree;
11823 
11824 // double dgL = 0.5*(dgV + dgA)/gLSM;
11825 // double dgR = 0.5*(dgV - dgA)/gRSM;
11826 
11827  double dsigmarat;
11828 
11829  /* VERY CRUDE APPROX. */
11830  //dsigmarat = 1.0 +
11831  // 2.0 * dkt -
11832  // 2.0 * (gLSM*gLSM*dgL + gRSM*gRSM*dgR)/(gLSM*gLSM + gRSM*gRSM);
11833 
11834  dsigmarat = 1.0;
11835 // ttH 100 TeV (from muttH func): NOT BOOSTED YET
11836  dsigmarat += +467438. * CHG / LambdaNP2
11837  -22519. * CG / LambdaNP2
11838  +880378. * CuG_33r / LambdaNP2
11839  -2.837 * deltaG_hff(quarks[TOP]).real()
11840  ;
11841 // Divided (linearized) by ttZ 100 TeV
11842  dsigmarat = dsigmarat - (
11843  -40869.4 * CHD / LambdaNP2
11844  -52607.9 * CHWB / LambdaNP2
11845  -90424.9 * CHG / LambdaNP2
11846  +432089. * CG / LambdaNP2
11847  +326525. * CuG_33r / LambdaNP2
11848  -2028.11 * CuW_33r / LambdaNP2
11849  +1679.85 * CuB_33r / LambdaNP2
11850  +1454.5 * CHQ1_11 / LambdaNP2
11851  +1065.27 * CHu_11 / LambdaNP2
11852  +82169.1 * CHu_33 / LambdaNP2
11853  -1229.16 * CHd_11 / LambdaNP2
11854  +6780.84 * CHQ3_11 / LambdaNP2
11855  -1.374 * DeltaGF()
11856  +4.242 * -0.5 * (CHQ1_33 - CHQ3_33) * v2_over_LambdaNP2
11857  );
11858 
11859  return dsigmarat * (BrHbbrat / BrZbbrat);
11860 
11861 }
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3429
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
const double & real() const
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3494
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
StandardModel trueSM
Definition: NPbase.h:1902
virtual double Gamma_Z() const
The total decay width of the boson, .
Definition: QCD.h:619
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
virtual double GammaZ(const Particle f) const
The partial decay width, .
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:2878
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
virtual double BR_Zf(const Particle f) const
The Branching ratio of the boson into a given fermion pair, .
Definition: NPbase.cpp:222
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ muttHZga()

double NPSMEFTd6::muttHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11930 of file NPSMEFTd6.cpp.

11931 {
11932  return muttH(sqrt_s) * BrHZgaRatio();
11933 
11934 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738

◆ muttHZZ()

double NPSMEFTd6::muttHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ}\)

Reimplemented from NPbase.

Definition at line 11966 of file NPSMEFTd6.cpp.

11967 {
11968  return muttH(sqrt_s) * BrHZZRatio();
11969 
11970 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267

◆ muttHZZ4l()

double NPSMEFTd6::muttHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12002 of file NPSMEFTd6.cpp.

12003 {
12004  return muttH(sqrt_s) * BrHZZ4lRatio();
12005 
12006 }
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:8267
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ muVBF()

double NPSMEFTd6::muVBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF}\)

Reimplemented from NPbase.

Definition at line 3192 of file NPSMEFTd6.cpp.

3193 {
3194  double mu = 1.0;
3195 
3196  double C1 = 0.0;
3197 
3198  if (sqrt_s == 1.96) {
3199 
3200  C1 = 0.0; // N.A.
3201 
3202  mu +=
3203  +120936. * (1. + eVBF_2_Hbox ) * CHbox / LambdaNP2
3204  -9422.68 * (1. + eVBF_2_HQ1_11 ) * CHQ1_11 / LambdaNP2
3205  -10683.8 * (1. + eVBF_2_Hu_11 ) * CHu_11 / LambdaNP2
3206  +4055.59 * (1. + eVBF_2_Hd_11 ) * CHd_11 / LambdaNP2
3207  -229691. * (1. + eVBF_2_HQ3_11 ) * CHQ3_11 / LambdaNP2
3208  -170093. * (1. + eVBF_2_HD ) * CHD / LambdaNP2
3209  +8971.22 * (1. + eVBF_2_HB ) * CHB / LambdaNP2
3210  -65827.6 * (1. + eVBF_2_HW ) * CHW / LambdaNP2
3211  -323514. * (1. + eVBF_2_HWB ) * CHWB / LambdaNP2
3212  +481332. * (1. + eVBF_2_HG ) * CHG / LambdaNP2
3213  +1255.16 * (1. + eVBF_2_DHB ) * CDHB / LambdaNP2
3214  -34956.7 * (1. + eVBF_2_DHW ) * CDHW / LambdaNP2
3215  -4.511 * (1. + eVBF_2_DeltaGF ) * DeltaGF()
3216  -3.481 * deltaMwd6()
3217  ;
3218 
3219  if (FlagQuadraticTerms) {
3220  //Add contributions that are quadratic in the effective coefficients
3221 
3222  mu += 0.0;
3223 
3224  }
3225 
3226  } else if (sqrt_s == 7.0) {
3227 
3228  C1 = 0.0065;
3229 
3230  mu +=
3231  +121582. * (1. + eVBF_78_Hbox ) * CHbox / LambdaNP2
3232  +13546.6 * (1. + eVBF_78_HQ1_11 ) * CHQ1_11 / LambdaNP2
3233  -27657.6 * (1. + eVBF_78_Hu_11 ) * CHu_11 / LambdaNP2
3234  +8892.12 * (1. + eVBF_78_Hd_11 ) * CHd_11 / LambdaNP2
3235  -411400. * (1. + eVBF_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
3236  -164286. * (1. + eVBF_78_HD ) * CHD / LambdaNP2
3237  -423.123 * (1. + eVBF_78_HB ) * CHB / LambdaNP2
3238  -89854. * (1. + eVBF_78_HW ) * CHW / LambdaNP2
3239  -312617. * (1. + eVBF_78_HWB ) * CHWB / LambdaNP2
3240  -82956.8 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3241  -279.08 * (1. + eVBF_78_DHB ) * CDHB / LambdaNP2
3242  -54861. * (1. + eVBF_78_DHW ) * CDHW / LambdaNP2
3243  -4.479 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3244  -3.22 * deltaMwd6()
3245  ;
3246 
3247  if (FlagQuadraticTerms) {
3248  //Add contributions that are quadratic in the effective coefficients
3249 
3250  mu += 0.0;
3251 
3252  }
3253 
3254  } else if (sqrt_s == 8.0) {
3255 
3256  C1 = 0.0065;
3257 
3258  mu +=
3259  +121042. * (1. + eVBF_78_Hbox ) * CHbox / LambdaNP2
3260  +12739.3 * (1. + eVBF_78_HQ1_11 ) * CHQ1_11 / LambdaNP2
3261  -28367.7 * (1. + eVBF_78_Hu_11 ) * CHu_11 / LambdaNP2
3262  +9134.21 * (1. + eVBF_78_Hd_11 ) * CHd_11 / LambdaNP2
3263  -423704. * (1. + eVBF_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
3264  -165182. * (1. + eVBF_78_HD ) * CHD / LambdaNP2
3265  -349.242 * (1. + eVBF_78_HB ) * CHB / LambdaNP2
3266  -87279.4 * (1. + eVBF_78_HW ) * CHW / LambdaNP2
3267  -313449. * (1. + eVBF_78_HWB ) * CHWB / LambdaNP2
3268  -69421.9 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3269  -373.338 * (1. + eVBF_78_DHB ) * CDHB / LambdaNP2
3270  -57028.1 * (1. + eVBF_78_DHW ) * CDHW / LambdaNP2
3271  -4.472 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3272  -3.138 * deltaMwd6()
3273  ;
3274 
3275  if (FlagQuadraticTerms) {
3276  //Add contributions that are quadratic in the effective coefficients
3277 
3278  mu += 0.0;
3279 
3280  }
3281  } else if (sqrt_s == 13.0) {
3282 
3283  C1 = 0.0064;
3284 
3285  mu +=
3286  +121798. * (1. + eVBF_1314_Hbox ) * CHbox / LambdaNP2
3287  +10339.7 * (1. + eVBF_1314_HQ1_11 ) * CHQ1_11 / LambdaNP2
3288  -30827.2 * (1. + eVBF_1314_Hu_11 ) * CHu_11 / LambdaNP2
3289  +10564.3 * (1. + eVBF_1314_Hd_11 ) * CHd_11 / LambdaNP2
3290  -466270. * (1. + eVBF_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
3291  -164119. * (1. + eVBF_1314_HD ) * CHD / LambdaNP2
3292  -61.471 * (1. + eVBF_1314_HB ) * CHB / LambdaNP2
3293  -82985.3 * (1. + eVBF_1314_HW ) * CHW / LambdaNP2
3294  -313815. * (1. + eVBF_1314_HWB ) * CHWB / LambdaNP2
3295  -36554. * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3296  -725.694 * (1. + eVBF_1314_DHB ) * CDHB / LambdaNP2
3297  -65253.4 * (1. + eVBF_1314_DHW ) * CDHW / LambdaNP2
3298  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3299  -3.109 * deltaMwd6()
3300  ;
3301 
3302  if (FlagQuadraticTerms) {
3303  //Add contributions that are quadratic in the effective coefficients
3304  mu += 0.0;
3305  }
3306 
3307  } else if (sqrt_s == 14.0) {
3308 
3309  C1 = 0.0064;
3310 
3311  mu +=
3312  +120948. * (1. + eVBF_1314_Hbox ) * CHbox / LambdaNP2
3313  +9896.36 * (1. + eVBF_1314_HQ1_11 ) * CHQ1_11 / LambdaNP2
3314  -31371. * (1. + eVBF_1314_Hu_11 ) * CHu_11 / LambdaNP2
3315  +10716.4 * (1. + eVBF_1314_Hd_11 ) * CHd_11 / LambdaNP2
3316  -473497. * (1. + eVBF_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
3317  -164672. * (1. + eVBF_1314_HD ) * CHD / LambdaNP2
3318  -60.253 * (1. + eVBF_1314_HB ) * CHB / LambdaNP2
3319  -83504.9 * (1. + eVBF_1314_HW ) * CHW / LambdaNP2
3320  -314059. * (1. + eVBF_1314_HWB ) * CHWB / LambdaNP2
3321  -33627.6 * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3322  -775.959 * (1. + eVBF_1314_DHB ) * CDHB / LambdaNP2
3323  -66336.3 * (1. + eVBF_1314_DHW ) * CDHW / LambdaNP2
3324  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3325  -3.193 * deltaMwd6()
3326  ;
3327 
3328  if (FlagQuadraticTerms) {
3329  //Add contributions that are quadratic in the effective coefficients
3330  mu += 0.0;
3331 
3332  }
3333 
3334  } else if (sqrt_s == 27.0) {
3335 
3336  C1 = 0.0; // N.A.
3337 
3338  mu +=
3339  +120777. * CHbox / LambdaNP2
3340  +6664.27 * CHQ1_11 / LambdaNP2
3341  -34230.7 * CHu_11 / LambdaNP2
3342  +12917.3 * CHd_11 / LambdaNP2
3343  -536216. * CHQ3_11 / LambdaNP2
3344  -163493. * CHD / LambdaNP2
3345  +58.33 * CHB / LambdaNP2
3346  -81360.5 * CHW / LambdaNP2
3347  -313026. * CHWB / LambdaNP2
3348  -16430. * CHG / LambdaNP2
3349  -1314.45 * CDHB / LambdaNP2
3350  -75884.6 * CDHW / LambdaNP2
3351  -4.475 * DeltaGF()
3352  -2.99 * deltaMwd6()
3353  ;
3354 
3355  if (FlagQuadraticTerms) {
3356  //Add contributions that are quadratic in the effective coefficients
3357  mu += 0.0;
3358 
3359  }
3360 
3361  } else if (sqrt_s == 100.0) {
3362 
3363  C1 = 0.0; // N.A.
3364 
3365  mu +=
3366  +121714. * CHbox / LambdaNP2
3367  -2261.73 * CHQ1_11 / LambdaNP2
3368  -42045.4 * CHu_11 / LambdaNP2
3369  +17539.2 * CHd_11 / LambdaNP2
3370  -674206. * CHQ3_11 / LambdaNP2
3371  -163344. * CHD / LambdaNP2
3372  +71.488 * CHB / LambdaNP2
3373  -90808.2 * CHW / LambdaNP2
3374  -312544. * CHWB / LambdaNP2
3375  -8165.65 * CHG / LambdaNP2
3376  -2615.48 * CDHB / LambdaNP2
3377  -96539.6 * CDHW / LambdaNP2
3378  -4.452 * DeltaGF()
3379  -2.949 * deltaMwd6()
3380  ;
3381 
3382  if (FlagQuadraticTerms) {
3383  //Add contributions that are quadratic in the effective coefficients
3384  mu += 0.0;
3385 
3386  }
3387 
3388  } else
3389  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBF()");
3390 
3391  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3392  mu += eVBFint + eVBFpar;
3393 
3394 // Linear contribution from Higgs self-coupling
3395  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3396 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3398 
3399  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3400 
3401  return mu;
3402 }
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double eVBF_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3681
double eVBF_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3694
double eVBF_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3709
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double eVBF_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3706
double eVBF_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3703
double eVBF_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3707
double eVBF_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3695
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double eVBF_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3685
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3640
double eVBF_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3687
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eVBF_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3672
double eVBF_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3674
double eVBF_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3671
double eVBF_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3673
double eVBF_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3683
double eVBF_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3686
double eVBF_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3700
double eVBF_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3689
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3641
double eVBF_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3701
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double eVBF_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3696
double eVBF_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3691
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double eVBF_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3676
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double eVBF_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3693
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double eVBF_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3704
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double eVBF_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3711
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double eVBF_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3692
double eVBF_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3702
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double eVBF_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3699
double eVBF_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3688
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double eVBF_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3677
double eVBF_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3682
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eVBF_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3697
double eVBF_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3678
double eVBF_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3679
double eVBF_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3680
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double eVBF_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3705
double eVBF_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3690
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
double eVBF_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3675
double eVBF_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3710
double eVBF_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3708

◆ muVBFgamma()

double NPSMEFTd6::muVBFgamma ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+\gamma}\)

Reimplemented from NPbase.

Definition at line 3407 of file NPSMEFTd6.cpp.

3408 {
3409  double mu = 1.0;
3410 
3411  double C1 = 0.0; //Use same values as VBF
3412 
3413  if (sqrt_s == 13.0) {
3414 
3415  C1 = 0.0064;
3416 
3417  mu +=
3418  +119630. * CHbox / LambdaNP2
3419  -501300. * CHQ3_11 / LambdaNP2
3420  -200890. * CHD / LambdaNP2
3421  +11852.5 * CHB / LambdaNP2
3422  -131586. * CHW / LambdaNP2
3423  -361991. * CHWB / LambdaNP2
3424  -18894.5 * CDHB / LambdaNP2
3425  -69025.4 * CDHW / LambdaNP2
3426  +23773.1 * CW / LambdaNP2
3427  -4.629 * DeltaGF()
3428  -5.637 * deltaMwd6()
3429  ;
3430 
3431  if (FlagQuadraticTerms) {
3432  //Add contributions that are quadratic in the effective coefficients
3433  mu += 0.0;
3434  }
3435 
3436  } else
3437  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBFgamma()");
3438 
3439  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy. Use same as VBF.)
3440  mu += eVBFint + eVBFpar;
3441 
3442 // Linear contribution from Higgs self-coupling
3443  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3444 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3446 
3447  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3448 
3449  return mu;
3450 }
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3640
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3641
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3430
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ muVBFHbb()

double NPSMEFTd6::muVBFHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,bb}\)

Reimplemented from NPbase.

Definition at line 12158 of file NPSMEFTd6.cpp.

12159 {
12160  return muVBF(sqrt_s) * BrHbbRatio();
12161 
12162 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905

◆ muVBFHgaga()

double NPSMEFTd6::muVBFHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11870 of file NPSMEFTd6.cpp.

11871 {
11872  return muVBF(sqrt_s) * BrHgagaRatio();
11873 
11874 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801

◆ muVBFHmumu()

double NPSMEFTd6::muVBFHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12086 of file NPSMEFTd6.cpp.

12087 {
12088  return muVBF(sqrt_s) * BrHmumuRatio();
12089 
12090 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827

◆ muVBFHtautau()

double NPSMEFTd6::muVBFHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12122 of file NPSMEFTd6.cpp.

12123 {
12124  return muVBF(sqrt_s) * BrHtautauRatio();
12125 
12126 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853

◆ muVBFHWW()

double NPSMEFTd6::muVBFHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW}\)

Reimplemented from NPbase.

Definition at line 12014 of file NPSMEFTd6.cpp.

12015 {
12016  return muVBF(sqrt_s) * BrHWWRatio();
12017 
12018 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muVBFHWW2l2v()

double NPSMEFTd6::muVBFHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12050 of file NPSMEFTd6.cpp.

12051 {
12052  return muVBF(sqrt_s) * BrHWW2l2vRatio();
12053 
12054 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192

◆ muVBFHZga()

double NPSMEFTd6::muVBFHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11906 of file NPSMEFTd6.cpp.

11907 {
11908  return muVBF(sqrt_s) * BrHZgaRatio();
11909 
11910 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738

◆ muVBFHZZ()

double NPSMEFTd6::muVBFHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ}\)

Reimplemented from NPbase.

Definition at line 11942 of file NPSMEFTd6.cpp.

11943 {
11944  return muVBF(sqrt_s) * BrHZZRatio();
11945 
11946 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192

◆ muVBFHZZ4l()

double NPSMEFTd6::muVBFHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 11978 of file NPSMEFTd6.cpp.

11979 {
11980  return muVBF(sqrt_s) * BrHZZ4lRatio();
11981 
11982 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ muVBFpVH()

double NPSMEFTd6::muVBFpVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+VH}\)

Reimplemented from NPbase.

Definition at line 8252 of file NPSMEFTd6.cpp.

8253 {
8254  double sigmaWH_SM = computeSigmaWH(sqrt_s);
8255  double sigmaZH_SM = computeSigmaZH(sqrt_s);
8256  double sigmaVBF_SM = computeSigmaVBF(sqrt_s);
8257  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
8258  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
8259  double sigmaVBF = muVBF(sqrt_s) * sigmaVBF_SM;
8260  double mu = ((sigmaWH + sigmaZH + sigmaVBF) / (sigmaWH_SM + sigmaZH_SM + sigmaVBF_SM));
8261 
8262  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8263 
8264  return mu;
8265 }
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3192
double computeSigmaZH(const double sqrt_s) const
The ZH production cross section in the Standard Model.
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
double computeSigmaVBF(const double sqrt_s) const
The VBF cross section in the Standard Model.
double computeSigmaWH(const double sqrt_s) const
The WH production cross section in the Standard Model.
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muVH()

double NPSMEFTd6::muVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH}\)

Reimplemented from NPbase.

Definition at line 8239 of file NPSMEFTd6.cpp.

8240 {
8241  double sigmaWH_SM = computeSigmaWH(sqrt_s);
8242  double sigmaZH_SM = computeSigmaZH(sqrt_s);
8243  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
8244  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
8245  double mu = ((sigmaWH + sigmaZH) / (sigmaWH_SM + sigmaZH_SM));
8246 
8247  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8248 
8249  return mu;
8250 }
double computeSigmaZH(const double sqrt_s) const
The ZH production cross section in the Standard Model.
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
double computeSigmaWH(const double sqrt_s) const
The WH production cross section in the Standard Model.
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muVHbb()

double NPSMEFTd6::muVHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,bb}\)

Reimplemented from NPbase.

Definition at line 12176 of file NPSMEFTd6.cpp.

12177 {
12178  return muVH(sqrt_s) * BrHbbRatio();
12179 
12180 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905

◆ muVHgaga()

double NPSMEFTd6::muVHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11888 of file NPSMEFTd6.cpp.

11889 {
11890  return muVH(sqrt_s) * BrHgagaRatio();
11891 
11892 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801

◆ muVHmumu()

double NPSMEFTd6::muVHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12104 of file NPSMEFTd6.cpp.

12105 {
12106  return muVH(sqrt_s) * BrHmumuRatio();
12107 
12108 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827

◆ muVHtautau()

double NPSMEFTd6::muVHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12140 of file NPSMEFTd6.cpp.

12141 {
12142  return muVH(sqrt_s) * BrHtautauRatio();
12143 
12144 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853

◆ muVHWW()

double NPSMEFTd6::muVHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW}\)

Reimplemented from NPbase.

Definition at line 12032 of file NPSMEFTd6.cpp.

12033 {
12034  return muVH(sqrt_s) * BrHWWRatio();
12035 
12036 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muVHWW2l2v()

double NPSMEFTd6::muVHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12068 of file NPSMEFTd6.cpp.

12069 {
12070  return muVH(sqrt_s) * BrHWW2l2vRatio();
12071 
12072 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239

◆ muVHZga()

double NPSMEFTd6::muVHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11924 of file NPSMEFTd6.cpp.

11925 {
11926  return muVH(sqrt_s) * BrHZgaRatio();
11927 
11928 }
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239

◆ muVHZZ()

double NPSMEFTd6::muVHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ}\)

Reimplemented from NPbase.

Definition at line 11960 of file NPSMEFTd6.cpp.

11961 {
11962  return muVH(sqrt_s) * BrHZZRatio();
11963 
11964 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239

◆ muVHZZ4l()

double NPSMEFTd6::muVHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 11996 of file NPSMEFTd6.cpp.

11997 {
11998  return muVH(sqrt_s) * BrHZZ4lRatio();
11999 
12000 }
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:8239
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ muWH()

double NPSMEFTd6::muWH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH}\)

Reimplemented from NPbase.

Definition at line 6530 of file NPSMEFTd6.cpp.

6531 {
6532  double mu = 1.0;
6533 
6534  double C1 = 0.0;
6535 
6536  if (sqrt_s == 1.96) {
6537 
6538  C1 = 0.0; // N.A.
6539 
6540  mu +=
6541  +121173. * (1. + eWH_2_Hbox ) * CHbox / LambdaNP2
6542  +1566788. * (1. + eWH_2_HQ3_11 ) * CHQ3_11 / LambdaNP2
6543  -160914. * (1. + eWH_2_HD ) * CHD / LambdaNP2
6544  +860916. * (1. + eWH_2_HW ) * CHW / LambdaNP2
6545  -286409. * (1. + eWH_2_HWB ) * CHWB / LambdaNP2
6546  +134641. * (1. + eWH_2_DHW ) * CDHW / LambdaNP2
6547  -3.31 * (1. + eWH_2_DeltaGF ) * DeltaGF()
6548  -2.199 * deltaMwd6()
6549  ;
6550 
6551  if (FlagQuadraticTerms) {
6552  //Add contributions that are quadratic in the effective coefficients
6553  mu += 0.0;
6554 
6555  }
6556 
6557  } else if (sqrt_s == 7.0) {
6558 
6559  C1 = 0.0106;
6560 
6561  mu +=
6562  +121015. * (1. + eWH_78_Hbox ) * CHbox / LambdaNP2
6563  +1792020. * (1. + eWH_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
6564  -159689. * (1. + eWH_78_HD ) * CHD / LambdaNP2
6565  +881065. * (1. + eWH_78_HW ) * CHW / LambdaNP2
6566  -283895. * (1. + eWH_78_HWB ) * CHWB / LambdaNP2
6567  +168173. * (1. + eWH_78_DHW ) * CDHW / LambdaNP2
6568  -3.273 * (1. + eWH_78_DeltaGF ) * DeltaGF()
6569  -2.143 * deltaMwd6()
6570  ;
6571 
6572  if (FlagQuadraticTerms) {
6573  //Add contributions that are quadratic in the effective coefficients
6574  mu += 0.0;
6575 
6576  }
6577 
6578  } else if (sqrt_s == 8.0) {
6579 
6580  C1 = 0.0105;
6581 
6582  mu +=
6583  +121226. * (1. + eWH_78_Hbox ) * CHbox / LambdaNP2
6584  +1830192. * (1. + eWH_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
6585  -159543. * (1. + eWH_78_HD ) * CHD / LambdaNP2
6586  +884671. * (1. + eWH_78_HW ) * CHW / LambdaNP2
6587  -283662. * (1. + eWH_78_HWB ) * CHWB / LambdaNP2
6588  +174061. * (1. + eWH_78_DHW ) * CDHW / LambdaNP2
6589  -3.278 * (1. + eWH_78_DeltaGF ) * DeltaGF()
6590  -2.147 * deltaMwd6()
6591  ;
6592 
6593  if (FlagQuadraticTerms) {
6594  //Add contributions that are quadratic in the effective coefficients
6595  mu += 0.0;
6596 
6597  }
6598 
6599  } else if (sqrt_s == 13.0) {
6600 
6601  C1 = 0.0103;
6602 
6603  mu +=
6604  +120439. * (1. + eWH_1314_Hbox ) * CHbox / LambdaNP2
6605  +1953200. * (1. + eWH_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
6606  -159847. * (1. + eWH_1314_HD ) * CHD / LambdaNP2
6607  +892264. * (1. + eWH_1314_HW ) * CHW / LambdaNP2
6608  -283830. * (1. + eWH_1314_HWB ) * CHWB / LambdaNP2
6609  +192168. * (1. + eWH_1314_DHW ) * CDHW / LambdaNP2
6610  -3.269 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
6611  -2.101 * deltaMwd6()
6612  ;
6613 
6614  if (FlagQuadraticTerms) {
6615  //Add contributions that are quadratic in the effective coefficients
6616  mu += 0.0;
6617 
6618  }
6619 
6620  } else if (sqrt_s == 14.0) {
6621 
6622  C1 = 0.0103;
6623 
6624  mu +=
6625  +120284. * (1. + eWH_1314_Hbox ) * CHbox / LambdaNP2
6626  +1971011. * (1. + eWH_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
6627  -159830. * (1. + eWH_1314_HD ) * CHD / LambdaNP2
6628  +893216. * (1. + eWH_1314_HW ) * CHW / LambdaNP2
6629  -283818. * (1. + eWH_1314_HWB ) * CHWB / LambdaNP2
6630  +194877. * (1. + eWH_1314_DHW ) * CDHW / LambdaNP2
6631  -3.272 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
6632  -2.103 * deltaMwd6()
6633  ;
6634 
6635  if (FlagQuadraticTerms) {
6636  //Add contributions that are quadratic in the effective coefficients
6637  mu += 0.0;
6638 
6639  }
6640 
6641  } else if (sqrt_s == 27.0) {
6642 
6643  C1 = 0.0; // N.A.
6644 
6645  mu +=
6646  +120696. * CHbox / LambdaNP2
6647  +2105646. * CHQ3_11 / LambdaNP2
6648  -159695. * CHD / LambdaNP2
6649  +900162. * CHW / LambdaNP2
6650  -283257. * CHWB / LambdaNP2
6651  +215592. * CDHW / LambdaNP2
6652  -3.256 * DeltaGF()
6653  -2.063 * deltaMwd6()
6654  ;
6655 
6656  if (FlagQuadraticTerms) {
6657  //Add contributions that are quadratic in the effective coefficients
6658  mu += 0.0;
6659 
6660  }
6661 
6662  } else if (sqrt_s == 100.0) {
6663 
6664  C1 = 0.0; // N.A.
6665 
6666  mu +=
6667  +121319. * CHbox / LambdaNP2
6668  +2294991. * CHQ3_11 / LambdaNP2
6669  -159242. * CHD / LambdaNP2
6670  +908130. * CHW / LambdaNP2
6671  -282574. * CHWB / LambdaNP2
6672  +245406. * CDHW / LambdaNP2
6673  -3.259 * DeltaGF()
6674  -2.047 * deltaMwd6()
6675  ;
6676 
6677  if (FlagQuadraticTerms) {
6678  //Add contributions that are quadratic in the effective coefficients
6679  mu += 0.0;
6680 
6681  }
6682 
6683  } else
6684  throw std::runtime_error("Bad argument in NPSMEFTd6::muWH()");
6685 
6686  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6687  mu += eWHint + eWHpar;
6688 
6689 // Linear contribution from Higgs self-coupling
6690  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
6691 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
6693 
6694  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6695 
6696  return mu;
6697 }
double eWH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3734
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double eWH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3721
double eWHpar
Parametric relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3643
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eWH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3714
double eWH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3718
double eWH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3723
double eWH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3716
double eWH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3724
double eWH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3725
double eWH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3722
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:2509
double eWH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3726
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double eWH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3733
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double eWH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3732
double eWH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3730
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double eWH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3713
double eWHint
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3642
double eWH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3729
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double eWH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3717
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double eWH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3715
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eWH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3727
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double eWH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3735
double eWH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3719
double eWH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3731
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832

◆ muWHbb()

double NPSMEFTd6::muWHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,bb}\)

Reimplemented from NPbase.

Definition at line 12170 of file NPSMEFTd6.cpp.

12171 {
12172  return muWH(sqrt_s) * BrHbbRatio();
12173 
12174 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905

◆ muWHgaga()

double NPSMEFTd6::muWHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11882 of file NPSMEFTd6.cpp.

11883 {
11884  return muWH(sqrt_s) * BrHgagaRatio();
11885 
11886 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801

◆ muWHmumu()

double NPSMEFTd6::muWHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12098 of file NPSMEFTd6.cpp.

12099 {
12100  return muWH(sqrt_s) * BrHmumuRatio();
12101 
12102 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827

◆ muWHtautau()

double NPSMEFTd6::muWHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12134 of file NPSMEFTd6.cpp.

12135 {
12136  return muWH(sqrt_s) * BrHtautauRatio();
12137 
12138 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853

◆ muWHWW()

double NPSMEFTd6::muWHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW}\)

Reimplemented from NPbase.

Definition at line 12026 of file NPSMEFTd6.cpp.

12027 {
12028  return muWH(sqrt_s) * BrHWWRatio();
12029 
12030 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muWHWW2l2v()

double NPSMEFTd6::muWHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12062 of file NPSMEFTd6.cpp.

12063 {
12064  return muWH(sqrt_s) * BrHWW2l2vRatio();
12065 
12066 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530

◆ muWHZga()

double NPSMEFTd6::muWHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11918 of file NPSMEFTd6.cpp.

11919 {
11920  return muWH(sqrt_s) * BrHZgaRatio();
11921 
11922 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738

◆ muWHZZ()

double NPSMEFTd6::muWHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ}\)

Reimplemented from NPbase.

Definition at line 11954 of file NPSMEFTd6.cpp.

11955 {
11956  return muWH(sqrt_s) * BrHZZRatio();
11957 
11958 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530

◆ muWHZZ4l()

double NPSMEFTd6::muWHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 11990 of file NPSMEFTd6.cpp.

11991 {
11992  return muWH(sqrt_s) * BrHZZ4lRatio();
11993 
11994 }
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6530
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ muZH()

double NPSMEFTd6::muZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH}\)

Reimplemented from NPbase.

Definition at line 6699 of file NPSMEFTd6.cpp.

6700 {
6701  double mu = 1.0;
6702 
6703  double C1 = 0.0;
6704 
6705  if (sqrt_s == 1.96) {
6706 
6707  C1 = 0.0; // N.A.
6708 
6709  mu +=
6710  +121197. * (1. + eZH_2_Hbox ) * CHbox / LambdaNP2
6711  -810445. * (1. + eZH_2_HQ1_11 ) * CHQ1_11 / LambdaNP2
6712  +529340. * (1. + eZH_2_Hu_11 ) * CHu_11 / LambdaNP2
6713  -69410.3 * (1. + eZH_2_Hd_11 ) * CHd_11 / LambdaNP2
6714  +1567161. * (1. + eZH_2_HQ3_11 ) * CHQ3_11 / LambdaNP2
6715  -16992.5 * (1. + eZH_2_HD ) * CHD / LambdaNP2
6716  +79314.5 * (1. + eZH_2_HB ) * CHB / LambdaNP2
6717  +711710. * (1. + eZH_2_HW ) * CHW / LambdaNP2
6718  +189054. * (1. + eZH_2_HWB ) * CHWB / LambdaNP2
6719  +9774.73 * (1. + eZH_2_DHB ) * CDHB / LambdaNP2
6720  +130777. * (1. + eZH_2_DHW ) * CDHW / LambdaNP2
6721  -2.535 * (1. + eZH_2_DeltaGF ) * DeltaGF()
6722  ;
6723 
6724  if (FlagQuadraticTerms) {
6725  //Add contributions that are quadratic in the effective coefficients
6726  mu += 0.0;
6727 
6728  }
6729 
6730  } else if (sqrt_s == 7.0) {
6731 
6732  C1 = 0.0123;
6733 
6734  mu +=
6735  +121069. * (1. + eZH_78_Hbox ) * CHbox / LambdaNP2
6736  -182215. * (1. + eZH_78_HQ1_11 ) * CHQ1_11 / LambdaNP2
6737  +421780. * (1. + eZH_78_Hu_11 ) * CHu_11 / LambdaNP2
6738  -139169. * (1. + eZH_78_Hd_11 ) * CHd_11 / LambdaNP2
6739  +1712111. * (1. + eZH_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
6740  -15395.4 * (1. + eZH_78_HD ) * CHD / LambdaNP2
6741  +87094.9 * (1. + eZH_78_HB ) * CHB / LambdaNP2
6742  +717388. * (1. + eZH_78_HW ) * CHW / LambdaNP2
6743  +203105. * (1. + eZH_78_HWB ) * CHWB / LambdaNP2
6744  +17532.4 * (1. + eZH_78_DHB ) * CDHB / LambdaNP2
6745  +152950. * (1. + eZH_78_DHW ) * CDHW / LambdaNP2
6746  -2.502 * (1. + eZH_78_DeltaGF ) * DeltaGF()
6747  ;
6748 
6749  if (FlagQuadraticTerms) {
6750  //Add contributions that are quadratic in the effective coefficients
6751  mu += 0.0;
6752 
6753  }
6754 
6755  } else if (sqrt_s == 8.0) {
6756 
6757  C1 = 0.0122;
6758 
6759  mu +=
6760  +121334. * (1. + eZH_78_Hbox ) * CHbox / LambdaNP2
6761  -176804. * (1. + eZH_78_HQ1_11 ) * CHQ1_11 / LambdaNP2
6762  +428587. * (1. + eZH_78_Hu_11 ) * CHu_11 / LambdaNP2
6763  -142508. * (1. + eZH_78_Hd_11 ) * CHd_11 / LambdaNP2
6764  +1747367. * (1. + eZH_78_HQ3_11 ) * CHQ3_11 / LambdaNP2
6765  -15002.7 * (1. + eZH_78_HD ) * CHD / LambdaNP2
6766  +87781.5 * (1. + eZH_78_HB ) * CHB / LambdaNP2
6767  +721405. * (1. + eZH_78_HW ) * CHW / LambdaNP2
6768  +204540. * (1. + eZH_78_HWB ) * CHWB / LambdaNP2
6769  +18868.6 * (1. + eZH_78_DHB ) * CDHB / LambdaNP2
6770  +158432. * (1. + eZH_78_DHW ) * CDHW / LambdaNP2
6771  -2.507 * (1. + eZH_78_DeltaGF ) * DeltaGF()
6772  ;
6773 
6774  if (FlagQuadraticTerms) {
6775  //Add contributions that are quadratic in the effective coefficients
6776  mu += 0.0;
6777 
6778  }
6779 
6780  } else if (sqrt_s == 13.0) {
6781 
6782  C1 = 0.0119;
6783 
6784  mu +=
6785  +121374. * (1. + eZH_1314_Hbox ) * CHbox / LambdaNP2
6786  -152273. * (1. + eZH_1314_HQ1_11 ) * CHQ1_11 / LambdaNP2
6787  +448168. * (1. + eZH_1314_Hu_11 ) * CHu_11 / LambdaNP2
6788  -155999. * (1. + eZH_1314_Hd_11 ) * CHd_11 / LambdaNP2
6789  +1862364. * (1. + eZH_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
6790  -15185. * (1. + eZH_1314_HD ) * CHD / LambdaNP2
6791  +88937.9 * (1. + eZH_1314_HB ) * CHB / LambdaNP2
6792  +728207. * (1. + eZH_1314_HW ) * CHW / LambdaNP2
6793  +207857. * (1. + eZH_1314_HWB ) * CHWB / LambdaNP2
6794  +21647.4 * (1. + eZH_1314_DHB ) * CDHB / LambdaNP2
6795  +175015. * (1. + eZH_1314_DHW ) * CDHW / LambdaNP2
6796  -2.506 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
6797  ;
6798 
6799  if (FlagQuadraticTerms) {
6800  //Add contributions that are quadratic in the effective coefficients
6801  mu += 0.0;
6802 
6803  }
6804 
6805  } else if (sqrt_s == 14.0) {
6806 
6807  C1 = 0.0118;
6808 
6809  mu +=
6810  +121437. * (1. + eZH_1314_Hbox ) * CHbox / LambdaNP2
6811  -147580. * (1. + eZH_1314_HQ1_11 ) * CHQ1_11 / LambdaNP2
6812  +450628. * (1. + eZH_1314_Hu_11 ) * CHu_11 / LambdaNP2
6813  -157625. * (1. + eZH_1314_Hd_11 ) * CHd_11 / LambdaNP2
6814  +1878132. * (1. + eZH_1314_HQ3_11 ) * CHQ3_11 / LambdaNP2
6815  -15299.4 * (1. + eZH_1314_HD ) * CHD / LambdaNP2
6816  +88761.8 * (1. + eZH_1314_HB ) * CHB / LambdaNP2
6817  +729243. * (1. + eZH_1314_HW ) * CHW / LambdaNP2
6818  +207707. * (1. + eZH_1314_HWB ) * CHWB / LambdaNP2
6819  +21958.9 * (1. + eZH_1314_DHB ) * CDHB / LambdaNP2
6820  +177300. * (1. + eZH_1314_DHW ) * CDHW / LambdaNP2
6821  -2.507 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
6822  ;
6823 
6824  if (FlagQuadraticTerms) {
6825  //Add contributions that are quadratic in the effective coefficients
6826  mu += 0.0;
6827 
6828  }
6829 
6830  } else if (sqrt_s == 27.0) {
6831 
6832  C1 = 0.0; // N.A.
6833 
6834  mu +=
6835  +121206. * CHbox / LambdaNP2
6836  -101865. * CHQ1_11 / LambdaNP2
6837  +468029. * CHu_11 / LambdaNP2
6838  -173377. * CHd_11 / LambdaNP2
6839  +2002478. * CHQ3_11 / LambdaNP2
6840  -15486.3 * CHD / LambdaNP2
6841  +89958. * CHB / LambdaNP2
6842  +735013. * CHW / LambdaNP2
6843  +211026. * CHWB / LambdaNP2
6844  +25604. * CDHB / LambdaNP2
6845  +196710. * CDHW / LambdaNP2
6846  -2.505 * DeltaGF()
6847  ;
6848 
6849  if (FlagQuadraticTerms) {
6850  //Add contributions that are quadratic in the effective coefficients
6851  mu += 0.0;
6852 
6853  }
6854 
6855  } else if (sqrt_s == 100.0) {
6856 
6857  C1 = 0.0; // N.A.
6858 
6859  mu +=
6860  +121269. * CHbox / LambdaNP2
6861  +90.68 * CHQ1_11 / LambdaNP2
6862  +484275. * CHu_11 / LambdaNP2
6863  -197878. * CHd_11 / LambdaNP2
6864  +2175601. * CHQ3_11 / LambdaNP2
6865  -14992.4 * CHD / LambdaNP2
6866  +91707.3 * CHB / LambdaNP2
6867  +741805. * CHW / LambdaNP2
6868  +215319. * CHWB / LambdaNP2
6869  +31435.6 * CDHB / LambdaNP2
6870  +223843. * CDHW / LambdaNP2
6871  -2.504 * DeltaGF()
6872  ;
6873 
6874  if (FlagQuadraticTerms) {
6875  //Add contributions that are quadratic in the effective coefficients
6876  mu += 0.0;
6877  }
6878 
6879  } else
6880  throw std::runtime_error("Bad argument in NPSMEFTd6::muZH()");
6881 
6882  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6883  mu += eZHint + eZHpar;
6884 
6885 // Linear contribution from Higgs self-coupling
6886  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
6887 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
6889 
6890  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6891 
6892  return mu;
6893 }
double eZH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3774
double eZH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3760
double eZH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3763
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double eZH_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3738
double eZH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3737
double eZH_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3756
double eZH_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3766
double eZH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3742
double eZH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3748
double eZH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3768
double eZH_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3759
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double eZH_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3753
double eZH_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3743
double eZH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3773
double eZH_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3764
double eZH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3758
double eZH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3747
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double eZH_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3739
double eZH_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3740
double eZH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3745
double eZH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3741
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double eZH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3744
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:2892
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double eZH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3761
double eZH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3754
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double eZHint
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3644
double eZH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3771
double eZH_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3769
double eZH_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3772
double eZH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3750
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
double eZH_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3765
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eZH_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3752
double eZH_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3751
double eZH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3755
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
double eZHpar
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3645
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double eZH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3770
double eZH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3767
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
double eZH_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3746
double eZH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3757

◆ muZHbb()

double NPSMEFTd6::muZHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,bb}\)

Reimplemented from NPbase.

Definition at line 12164 of file NPSMEFTd6.cpp.

12165 {
12166  return muZH(sqrt_s) * BrHbbRatio();
12167 
12168 }
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9905
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHgaga()

double NPSMEFTd6::muZHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 11876 of file NPSMEFTd6.cpp.

11877 {
11878  return muZH(sqrt_s) * BrHgagaRatio();
11879 
11880 }
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9801
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHmumu()

double NPSMEFTd6::muZHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 12092 of file NPSMEFTd6.cpp.

12093 {
12094  return muZH(sqrt_s) * BrHmumuRatio();
12095 
12096 }
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9827
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHtautau()

double NPSMEFTd6::muZHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 12128 of file NPSMEFTd6.cpp.

12129 {
12130  return muZH(sqrt_s) * BrHtautauRatio();
12131 
12132 }
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9853
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHWW()

double NPSMEFTd6::muZHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW}\)

Reimplemented from NPbase.

Definition at line 12020 of file NPSMEFTd6.cpp.

12021 {
12022  return muZH(sqrt_s) * BrHWWRatio();
12023 
12024 }
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9267

◆ muZHWW2l2v()

double NPSMEFTd6::muZHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 12056 of file NPSMEFTd6.cpp.

12057 {
12058  return muZH(sqrt_s) * BrHWW2l2vRatio();
12059 
12060 }
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9299
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHZga()

double NPSMEFTd6::muZHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 11912 of file NPSMEFTd6.cpp.

11913 {
11914  return muZH(sqrt_s) * BrHZgaRatio();
11915 
11916 }
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9738
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHZZ()

double NPSMEFTd6::muZHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ}\)

Reimplemented from NPbase.

Definition at line 11948 of file NPSMEFTd6.cpp.

11949 {
11950  return muZH(sqrt_s) * BrHZZRatio();
11951 
11952 }
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9425
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699

◆ muZHZZ4l()

double NPSMEFTd6::muZHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 11984 of file NPSMEFTd6.cpp.

11985 {
11986  return muZH(sqrt_s) * BrHZZ4lRatio();
11987 
11988 }
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:6699
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:9455

◆ Mw()

double NPSMEFTd6::Mw ( ) const
virtual

The mass of the \(W\) boson, \(M_W\).

Returns
\(M_W\) in GeV

Reimplemented from NPbase.

Definition at line 2501 of file NPSMEFTd6.cpp.

2502 {
2503  return (trueSM.Mw() - Mw_tree() / 4.0 / (cW2_tree - sW2_tree)
2504  *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
2506  + 2.0 * sW2_tree * DeltaGF()));
2507 }
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2356
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
StandardModel trueSM
Definition: NPbase.h:1902
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
virtual double Mw() const
The SM prediction for the -boson mass in the on-shell scheme, .
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double Mw_tree() const
The tree-level mass of the boson, .
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440

◆ obliqueS()

double NPSMEFTd6::obliqueS ( ) const
virtual

The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)

Returns
the value of \(S\)

Reimplemented from NPbase.

Definition at line 2361 of file NPSMEFTd6.cpp.

2362 {
2363  return (4.0 * sW_tree * cW_tree * CHWB / alphaMz() * v2_over_LambdaNP2);
2364 }
double alphaMz() const
The electromagnetic coupling at the -mass scale, .
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440

◆ obliqueT()

double NPSMEFTd6::obliqueT ( ) const
virtual

The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)

Returns
the value of \(T\)

Reimplemented from NPbase.

Definition at line 2366 of file NPSMEFTd6.cpp.

2367 {
2368  return (-CHD / 2.0 / alphaMz() * v2_over_LambdaNP2);
2369 }
double alphaMz() const
The electromagnetic coupling at the -mass scale, .
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ obliqueU()

double NPSMEFTd6::obliqueU ( ) const
virtual

The oblique parameter \(U\).

Returns
the value of \(U\)

Reimplemented from NPbase.

Definition at line 2371 of file NPSMEFTd6.cpp.

2372 {
2373  return 0.0;
2374 }

◆ obliqueW()

double NPSMEFTd6::obliqueW ( ) const
virtual

The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)

Returns
the value of \(W\)

Reimplemented from NPbase.

Definition at line 2376 of file NPSMEFTd6.cpp.

2377 {
2378  return (- g2_tree * g2_tree * C2W * v2_over_LambdaNP2 / 2.0);
2379 }
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3811
double C2W
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3432
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ obliqueY()

double NPSMEFTd6::obliqueY ( ) const
virtual

The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)

Returns
the value of \(Y\)

Reimplemented from NPbase.

Definition at line 2381 of file NPSMEFTd6.cpp.

2382 {
2383  return (- g2_tree * g2_tree * C2B * v2_over_LambdaNP2 / 2.0);
2384 }
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3811
double C2B
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3431
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801

◆ PostUpdate()

bool NPSMEFTd6::PostUpdate ( )
virtual

The post-update method for NPSMEFTd6.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns
a boolean that is true if the execution is successful

Reimplemented from NPbase.

Definition at line 789 of file NPSMEFTd6.cpp.

790 {
791  if (!NPbase::PostUpdate()) return (false);
792 
793 // 0) Post-update operations not involving SM nor NP parameters
794  if (!FlagHiggsSM) {
795  cHSM = 0.0;
796  } else {
797  cHSM = 1.0;
798  }
799 
800  if (!FlagLoopHd6) {
801  cLHd6 = 0.0;
802  } else {
803  cLHd6 = 1.0;
804  }
805 
807  cLH3d62 = 1.0;
808  } else {
809  cLH3d62 = 0.0;
810  }
811 
812 // 1) Post-update operations involving SM parameters only
814  v2 = v() * v();
816  aleMz = alphaMz();
817  eeMz = sqrt( 4.0 * M_PI * aleMz );
818  eeMz2 = eeMz*eeMz;
819  cW_tree = Mw_tree() / Mz;
821  sW2_tree = 1.0 - cW2_tree;
822  sW_tree = sqrt(sW2_tree);
823 
824  g1_tree = eeMz/cW_tree;
825  g2_tree = eeMz/sW_tree;
826 
827  lambdaH_tree = mHl*mHl/2.0/v2;
828 
830  gZlL = (leptons[ELECTRON].getIsospin()) - (leptons[ELECTRON].getCharge())*sW2_tree;
832  gZuL = (quarks[UP].getIsospin()) - (quarks[UP].getCharge())*sW2_tree;
833  gZuR = - (quarks[UP].getCharge()) * sW2_tree;
834  gZdL = (quarks[DOWN].getIsospin()) - (quarks[DOWN].getCharge())*sW2_tree;
835  gZdR = - (quarks[DOWN].getCharge()) * sW2_tree;
836 
837  UevL = 1.0; // Neglect PMNS effects
838  VudL = 1.0; // Neglect CKM effects
839 
840  Yuke = sqrt(2.) * (leptons[ELECTRON].getMass()) / v();
841  Yukmu = sqrt(2.) * (leptons[MU].getMass()) / v();
842  Yuktau = sqrt(2.) * (leptons[TAU].getMass()) / v();
843  Yuku = sqrt(2.) * (quarks[UP].getMass()) / v();
844  Yukc = sqrt(2.) * (quarks[CHARM].getMass()) / v();
845  Yukt = sqrt(2.) * mtpole / v();
846  Yukd = sqrt(2.) * (quarks[DOWN].getMass()) / v();
847  Yuks = sqrt(2.) * (quarks[STRANGE].getMass()) / v();
848  Yukb = sqrt(2.) * (quarks[BOTTOM].getMass()) / v();
849 
850  dZH = -(9.0/16.0)*( GF*mHl*mHl/sqrt(2.0)/M_PI/M_PI )*( 2.0*M_PI/3.0/sqrt(3.0) - 1.0 );
851 
852 // 2) Post-update operations related to assumptions in the form of the dimension-6 operators
853  if (FlagFlavU3OfX || FlagUnivOfX) {
854 
855  if (FlagUnivOfX) {
856  CeH_11r = CuH_33r;
857  CeH_22r = CuH_33r;
858  CeH_33r = CuH_33r;
859 
860  CuH_11r = CuH_33r;
861  CuH_22r = CuH_33r;
862  // CuH_33r = CuH_33r;
863 
864  CdH_11r = CuH_33r;
865  CdH_22r = CuH_33r;
866  CdH_33r = CuH_33r;
867 
868  // Currently OfV are only implemented for u quarks so nothing else is needed to apply universality.
869  }
870 
871  CeH_11r = Yuke * CeH_11r;
872  CeH_22r = Yukmu * CeH_22r;
873  CeH_33r = Yuktau * CeH_33r;
874 
875  CuH_11r = Yuku * CuH_11r;
876  CuH_22r = Yukc * CuH_22r;
877  CuH_33r = Yukt * CuH_33r;
878 
879  CdH_11r = Yukd * CdH_11r;
880  CdH_22r = Yuks * CdH_22r;
881  CdH_33r = Yukb * CdH_33r;
882 
883  CuG_11r = Yuku * CuG_11r;
884  CuG_22r = Yukc * CuG_22r;
885  CuG_33r = Yukt * CuG_33r;
886 
887  CuW_11r = Yuku * CuW_11r;
888  CuW_22r = Yukc * CuW_22r;
889  CuW_33r = Yukt * CuW_33r;
890 
891  CuB_11r = Yuku * CuB_11r;
892  CuB_22r = Yukc * CuB_22r;
893  CuB_33r = Yukt * CuB_33r;
894  }
895 
896 // C2B and C2W are incorporated by change of basis transformation:
897 // Write here, before working with the dim 6 interactions,
898 // the contributions from O2W and O2B to the other operators.
899 // WARNING: Ignoring contributions to 4 fermion-processes for the moment. IMPORTANT FOR LEP2
900 
901 // WARNING: if some of the parameters below, e.g. CHL1_11, are not floating in the fit this will
902 // create a problem since the value generated below CHL1_11 will propagate to the next iteration
903 // generating an uncontrolled value of the parameter.
904 // (This is so because SetParameters is not called for non-floating parameters.)
905 // Possible fix: Not modify model parameters but save everything into internal replicas
906 // of each model relevant model par. Those then have to be used in the calculations.
907 // Comment out the following lines until this is resolved
908 // CHL1_11 = CHL1_11 - (g1_tree*g1_tree/2.0) * C2B;
909 // CHL1_22 = CHL1_22 - (g1_tree*g1_tree/2.0) * C2B;
910 // CHL1_33 = CHL1_33 - (g1_tree*g1_tree/2.0) * C2B;
911 // CHL3_11 = CHL3_11 + (g2_tree*g2_tree/2.0) * C2W;
912 // CHL3_22 = CHL3_22 + (g2_tree*g2_tree/2.0) * C2W;
913 // CHL3_33 = CHL3_33 + (g2_tree*g2_tree/2.0) * C2W;
914 
915 // CHQ1_11 = CHQ1_11 + (g1_tree*g1_tree/6.0) * C2B;
916 // CHQ1_22 = CHQ1_22 + (g1_tree*g1_tree/6.0) * C2B;
917 // CHQ1_33 = CHQ1_33 + (g1_tree*g1_tree/6.0) * C2B;
918 // CHQ3_11 = CHQ3_11 + (g2_tree*g2_tree/2.0) * C2W;
919 // CHQ3_22 = CHQ3_22 + (g2_tree*g2_tree/2.0) * C2W;
920 // CHQ3_33 = CHQ3_33 + (g2_tree*g2_tree/2.0) * C2W;
921 
922 // CHe_11 = CHe_11 - (g1_tree*g1_tree) * C2B;
923 // CHe_22 = CHe_22 - (g1_tree*g1_tree) * C2B;
924 // CHe_33 = CHe_33 - (g1_tree*g1_tree) * C2B;
925 
926 // CHu_11 = CHu_11 + (2.0*g1_tree*g1_tree/3.0) * C2B;
927 // CHu_22 = CHu_22 + (2.0*g1_tree*g1_tree/3.0) * C2B;
928 // CHu_33 = CHu_33 + (2.0*g1_tree*g1_tree/3.0) * C2B;
929 
930 // CHd_11 = CHd_11 - (g1_tree*g1_tree/3.0) * C2B;
931 // CHd_22 = CHd_22 - (g1_tree*g1_tree/3.0) * C2B;
932 // CHd_33 = CHd_33 - (g1_tree*g1_tree/3.0) * C2B;
933 
934 // CW = CW + g2_tree * C2W;
935 
936 // CHbox = CHbox + (g1_tree*g1_tree/4.0) * C2B + (3.0*g2_tree*g2_tree/4.0) * C2W;
937 // CHD = CHD + (g1_tree*g1_tree/4.0) * C2B;
938 // CH = CH + (2.0*g2_tree*g2_tree*lambdaH_tree) * C2W;
939 
940 // CeH_11r = CeH_11r + (g2_tree*g2_tree*Yuke) * C2W;
941 // CeH_22r = CeH_22r + (g2_tree*g2_tree*Yukmu) * C2W;
942 // CeH_33r = CeH_33r + (g2_tree*g2_tree*Yuktau) * C2W;
943 
944 // CuH_11r = CuH_11r + (g2_tree*g2_tree*Yuku) * C2W;
945 // CuH_22r = CuH_22r + (g2_tree*g2_tree*Yukc) * C2W;
946 // CuH_33r = CuH_33r + (g2_tree*g2_tree*Yukt) * C2W;
947 
948 // CdH_11r = CdH_11r + (g2_tree*g2_tree*Yukd) * C2W;
949 // CdH_22r = CdH_22r + (g2_tree*g2_tree*Yuks) * C2W;
950 // CdH_33r = CdH_33r + (g2_tree*g2_tree*Yukb) * C2W;
951 
952 // CLL_1221 = CLL_1221 + (g2_tree*g2_tree/2.0) * C2W;
953 // CLL_2112 = CLL_1221;
954 
955 
956 // 3) Post-update operations working directly with the dimension six operators
957  if (FlagRotateCHWCHB) {
960  } else {
963  }
964 
967  delta_AZ = 2.0 * sW_tree * cW_tree * (CHW - CHB) * v2_over_LambdaNP2
969  delta_h = (-CHD / 4.0 + CHbox) * v2_over_LambdaNP2;
970 
971 // Calculation of some quantities repeteadly used in the code
972 
973 // NP corrections to Total Higgs width
975 
976  if (FlagQuadraticTerms) {
978  } else {
979  dGammaHTotR2 = 0.0;
980  }
981 
982 // Total: to be used in BR functions to check positivity
984 
986 
987  return (true);
988 }
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
virtual double deltaGammaTotalRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
Definition: NPSMEFTd6.cpp:9948
double lambdaH_tree
The SM tree level value of the scalar quartic coupling in the potential.
Definition: NPSMEFTd6.h:3826
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double VudL
The tree level value of the couplings in the SM. (Neglecting CKM effects.)
Definition: NPSMEFTd6.h:3819
double Yukd
Definition: NPSMEFTd6.h:3838
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3822
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3823
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3824
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
double UevL
The tree level value of the couplings in the SM. (Neglecting PMNS effects.)
Definition: NPSMEFTd6.h:3818
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3567
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3543
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double alphaMz() const
The electromagnetic coupling at the -mass scale, .
bool FlagUnivOfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and ...
Definition: NPSMEFTd6.h:3907
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes...
Definition: NPSMEFTd6.h:3830
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3579
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
double Yuks
Definition: NPSMEFTd6.h:3838
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3808
virtual double deltaGammaTotalRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model...
Definition: NPSMEFTd6.cpp:9970
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CHWHB_gagaorth
The combination of dimension-6 operator coefficients .
Definition: NPSMEFTd6.h:3437
Matching< NPSMEFTd6Matching, NPSMEFTd6 > NPSMEFTd6M
Definition: NPSMEFTd6.h:3427
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3555
double gZdR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3816
Definition: QCD.h:615
double GF
The Fermi constant in .
T & getObj()
Definition: Matching.h:16
double gZuL
Definition: NPSMEFTd6.h:3815
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3811
double Yuktau
SM lepton Yukawas.
Definition: NPSMEFTd6.h:3836
double mHl
The Higgs mass in GeV.
double dGammaHTotR1
Definition: NPSMEFTd6.h:3841
double Yukb
SM d-quark Yukawas.
Definition: NPSMEFTd6.h:3838
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:3904
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3519
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3807
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3558
double Yuke
Definition: NPSMEFTd6.h:3836
double dGammaHTotR2
Definition: NPSMEFTd6.h:3841
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3570
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:3821
double Mz
The mass of the boson in GeV.
double gZlL
Definition: NPSMEFTd6.h:3814
double gZvL
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3813
Definition: QCD.h:607
double mtpole
The pole mass of the top quark.
Definition: QCD.h:1214
double g1_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3810
double Yukt
SM u-quark Yukawas.
Definition: NPSMEFTd6.h:3837
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:3802
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients...
Definition: NPSMEFTd6.h:3906
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:3791
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
Definition: QCD.h:616
double Yukc
Definition: NPSMEFTd6.h:3837
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3531
bool FlagHiggsSM
A boolean flag that is true if including dependence on small variations of the SM parameters (depende...
Definition: NPSMEFTd6.h:3908
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
double Yuku
Definition: NPSMEFTd6.h:3837
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3546
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3582
Particle leptons[6]
An array of Particle objects for the leptons.
double gZlR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3814
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:3841
virtual bool PostUpdate()
The postupdate method for NPbase.
Definition: NPbase.cpp:23
double Yukmu
Definition: NPSMEFTd6.h:3836
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
virtual double v() const
The value of at any scale with the number of flavours and full EW corrections. ...
double gZuR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:3815
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:1222
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
virtual double Mw_tree() const
The tree-level mass of the boson, .
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:3909
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
bool FlagLoopH3d6Quad
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables...
Definition: NPSMEFTd6.h:3910
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double gZdL
Definition: NPSMEFTd6.h:3816
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:3800
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:3828
Definition: QCD.h:605
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:3804
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:3634
double CHWHB_gaga
The combination of dimension-6 operator coefficients entering in : .
Definition: NPSMEFTd6.h:3436
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3834
void updateNPSMEFTd6Parameters()
Updates to new FlavourWilsonCoefficient parameter sets.
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:3832
complex sqrt(const complex &z)
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ ppZHprobe()

double NPSMEFTd6::ppZHprobe ( const double  sqrt_s) const
virtual

The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.

Returns
\(g_p^Z\)

Reimplemented from NPbase.

Definition at line 12587 of file NPSMEFTd6.cpp.

12588 {
12589 
12590  double gpZ=0.0;
12591 
12592  double ghZuL,ghZdL,ghZuR,ghZdR;
12593 
12594  // In the Warsaw basis the contact interactions are generated only by CHF ops but
12595  // in the modified basis ODHB, ODHW also contribute
12596 
12597  ghZuL = -(eeMz/sW_tree/cW_tree)*(CHQ1_11 - CHQ3_11 + g1_tree * (1.0/12.0) * CDHB - (g2_tree/4.0) * CDHW) * v2_over_LambdaNP2;
12598  ghZdL = -(eeMz/sW_tree/cW_tree)*(CHQ1_11 + CHQ3_11 + g1_tree * (1.0/12.0) * CDHB + (g2_tree/4.0) * CDHW) * v2_over_LambdaNP2;
12599  ghZuR = -(eeMz/sW_tree/cW_tree)*(CHu_11 + g1_tree * (1.0/3.0) * CDHB) * v2_over_LambdaNP2;
12600  ghZdR = -(eeMz/sW_tree/cW_tree)*(CHd_11 - g1_tree * (1.0/6.0) * CDHB) * v2_over_LambdaNP2;
12601 
12602  if (sqrt_s == 14.0) {
12603 
12604  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
12605 
12606  } else if (sqrt_s == 27.0) {
12607  // Use the same as for 14 TeV for the moment
12608 
12609  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
12610 
12611  } else if (sqrt_s == 100.0) {
12612 
12613  gpZ = ghZuL - 0.90 * ghZdL - 0.45 * ghZuR + 0.17 * ghZdR;
12614 
12615  } else
12616  throw std::runtime_error("Bad argument in NPSMEFTd6::ppZHprobe()");
12617 
12618 
12619  return gpZ;
12620 
12621 }
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:3803
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:3806
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3811
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double g1_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:3810
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:3801
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:3805
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471

◆ setFlag()

bool NPSMEFTd6::setFlag ( const std::string  name,
const bool  value 
)
virtual

A method to set a flag of NPSMEFTd6.

Parameters
[in]namename of a model flag
[in]valuethe boolean to be assigned to the flag specified by name
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2135 of file NPSMEFTd6.cpp.

2136 {
2137  bool res = false;
2138  if (name.compare("QuadraticTerms") == 0) {
2139  FlagQuadraticTerms = value;
2140  if(value) setModelLinearized(false);
2141  res = true;
2142  } else if (name.compare("RotateCHWCHB") == 0) {
2143  FlagRotateCHWCHB = value;
2144  res = true;
2145  } else if (name.compare("PartialQFU") == 0) {
2146  FlagPartialQFU = value;
2147  res = true;
2148  } else if (name.compare("FlavU3OfX") == 0) {
2149  FlagFlavU3OfX = value;
2150  res = true;
2151  } else if (name.compare("UnivOfX") == 0) {
2152  FlagUnivOfX = value;
2153  res = true;
2154  } else if (name.compare("HiggsSM") == 0) {
2155  FlagHiggsSM = value;
2156  res = true;
2157  } else if (name.compare("LoopHd6") == 0) {
2158  FlagLoopHd6 = value;
2159  res = true;
2160  } else if (name.compare("LoopH3d6Quad") == 0) {
2161  FlagLoopH3d6Quad = value;
2162  res = true;
2163  } else
2164  res = NPbase::setFlag(name, value);
2165 
2166  return (res);
2167 }
bool FlagUnivOfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and ...
Definition: NPSMEFTd6.h:3907
std::string name
The name of the model.
Definition: Model.h:246
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:3904
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients...
Definition: NPSMEFTd6.h:3906
bool FlagHiggsSM
A boolean flag that is true if including dependence on small variations of the SM parameters (depende...
Definition: NPSMEFTd6.h:3908
bool FlagPartialQFU
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd fa...
Definition: NPSMEFTd6.h:3905
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:3909
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on...
Definition: NPSMEFTd6.h:3903
bool FlagLoopH3d6Quad
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables...
Definition: NPSMEFTd6.h:3910
void setModelLinearized(bool linearized=true)
Definition: Model.h:222
virtual bool setFlag(const std::string name, const bool value)
A method to set a flag of StandardModel.

◆ setParameter()

void NPSMEFTd6::setParameter ( const std::string  name,
const double &  value 
)
protectedvirtual

A method to set the value of a parameter of the model.

Parameters
[in]namename of a model parameter
[in]valuethe value to be assigned to the parameter specified by name

Reimplemented from StandardModel.

Definition at line 990 of file NPSMEFTd6.cpp.

991 {
992  if (name.compare("CG") == 0)
993  CG = value;
994  else if (name.compare("CW") == 0)
995  CW = value;
996  else if (name.compare("C2B") == 0)
997  C2B = value;
998  else if (name.compare("C2W") == 0)
999  C2W = value;
1000  else if (name.compare("CHG") == 0)
1001  CHG = value;
1002  else if (name.compare("CHW") == 0)
1003  CHW = value;
1004  else if (name.compare("CHB") == 0)
1005  CHB = value;
1006  else if (name.compare("CHWHB_gaga") == 0)
1007  CHWHB_gaga = value;
1008  else if (name.compare("CHWHB_gagaorth") == 0)
1009  CHWHB_gagaorth = value;
1010  else if (name.compare("CDHB") == 0)
1011  CDHB = value;
1012  else if (name.compare("CDHW") == 0)
1013  CDHW = value;
1014  else if (name.compare("CHWB") == 0)
1015  CHWB = value;
1016  else if (name.compare("CHD") == 0)
1017  CHD = value;
1018  else if (name.compare("CHbox") == 0)
1019  CHbox = value;
1020  else if (name.compare("CH") == 0)
1021  CH = value;
1022  else if (name.compare("CHL1_11") == 0)
1023  CHL1_11 = value;
1024  else if (name.compare("CHL1_12r") == 0)
1025  CHL1_12r = value;
1026  else if (name.compare("CHL1_13r") == 0)
1027  CHL1_13r = value;
1028  else if (name.compare("CHL1_22") == 0)
1029  CHL1_22 = value;
1030  else if (name.compare("CHL1_23r") == 0)
1031  CHL1_23r = value;
1032  else if (name.compare("CHL1_33") == 0)
1033  CHL1_33 = value;
1034  else if (name.compare("CHL1_12i") == 0)
1035  CHL1_12i = value;
1036  else if (name.compare("CHL1_13i") == 0)
1037  CHL1_13i = value;
1038  else if (name.compare("CHL1_23i") == 0)
1039  CHL1_23i = value;
1040  else if (name.compare("CHL1") == 0) {
1041  CHL1_11 = value;
1042  CHL1_12r = 0.0;
1043  CHL1_13r = 0.0;
1044  CHL1_22 = value;
1045  CHL1_23r = 0.0;
1046  CHL1_33 = value;
1047  CHL1_12i = 0.0;
1048  CHL1_13i = 0.0;
1049  CHL1_23i = 0.0;
1050  } else if (name.compare("CHL3_11") == 0)
1051  CHL3_11 = value;
1052  else if (name.compare("CHL3_12r") == 0)
1053  CHL3_12r = value;
1054  else if (name.compare("CHL3_13r") == 0)
1055  CHL3_13r = value;
1056  else if (name.compare("CHL3_22") == 0)
1057  CHL3_22 = value;
1058  else if (name.compare("CHL3_23r") == 0)
1059  CHL3_23r = value;
1060  else if (name.compare("CHL3_33") == 0)
1061  CHL3_33 = value;
1062  else if (name.compare("CHL3_12i") == 0)
1063  CHL3_12i = value;
1064  else if (name.compare("CHL3_13i") == 0)
1065  CHL3_13i = value;
1066  else if (name.compare("CHL3_23i") == 0)
1067  CHL3_23i = value;
1068  else if (name.compare("CHL3") == 0) {
1069  CHL3_11 = value;
1070  CHL3_12r = 0.0;
1071  CHL3_13r = 0.0;
1072  CHL3_22 = value;
1073  CHL3_23r = 0.0;
1074  CHL3_33 = value;
1075  CHL3_12i = 0.0;
1076  CHL3_13i = 0.0;
1077  CHL3_23i = 0.0;
1078  } else if (name.compare("CHe_11") == 0)
1079  CHe_11 = value;
1080  else if (name.compare("CHe_12r") == 0)
1081  CHe_12r = value;
1082  else if (name.compare("CHe_13r") == 0)
1083  CHe_13r = value;
1084  else if (name.compare("CHe_22") == 0)
1085  CHe_22 = value;
1086  else if (name.compare("CHe_23r") == 0)
1087  CHe_23r = value;
1088  else if (name.compare("CHe_33") == 0)
1089  CHe_33 = value;
1090  else if (name.compare("CHe_12i") == 0)
1091  CHe_12i = value;
1092  else if (name.compare("CHe_13i") == 0)
1093  CHe_13i = value;
1094  else if (name.compare("CHe_23i") == 0)
1095  CHe_23i = value;
1096  else if (name.compare("CHe") == 0) {
1097  CHe_11 = value;
1098  CHe_12r = 0.0;
1099  CHe_13r = 0.0;
1100  CHe_22 = value;
1101  CHe_23r = 0.0;
1102  CHe_33 = value;
1103  CHe_12i = 0.0;
1104  CHe_13i = 0.0;
1105  CHe_23i = 0.0;
1106  } else if (name.compare("CHQ1_11") == 0) {
1107  CHQ1_11 = value;
1108  if (FlagPartialQFU){
1109  CHQ1_22 = value;
1110  }
1111  } else if (name.compare("CHQ1_12r") == 0)
1112  CHQ1_12r = value;
1113  else if (name.compare("CHQ1_13r") == 0)
1114  CHQ1_13r = value;
1115  else if (name.compare("CHQ1_22") == 0) {
1116  if (!FlagPartialQFU){
1117  CHQ1_22 = value;
1118  }
1119  } else if (name.compare("CHQ1_23r") == 0)
1120  CHQ1_23r = value;
1121  else if (name.compare("CHQ1_33") == 0)
1122  CHQ1_33 = value;
1123  else if (name.compare("CHQ1_12i") == 0)
1124  CHQ1_12i = value;
1125  else if (name.compare("CHQ1_13i") == 0)
1126  CHQ1_13i = value;
1127  else if (name.compare("CHQ1_23i") == 0)
1128  CHQ1_23i = value;
1129  else if (name.compare("CHQ1") == 0) {
1130  CHQ1_11 = value;
1131  CHQ1_12r = 0.0;
1132  CHQ1_13r = 0.0;
1133  CHQ1_22 = value;
1134  CHQ1_23r = 0.0;
1135  CHQ1_33 = value;
1136  CHQ1_12i = 0.0;
1137  CHQ1_13i = 0.0;
1138  CHQ1_23i = 0.0;
1139  } else if (name.compare("CHQ3_11") == 0){
1140  CHQ3_11 = value;
1141  if (FlagPartialQFU){
1142  CHQ3_22 = value;
1143  }
1144  } else if (name.compare("CHQ3_12r") == 0)
1145  CHQ3_12r = value;
1146  else if (name.compare("CHQ3_13r") == 0)
1147  CHQ3_13r = value;
1148  else if (name.compare("CHQ3_22") == 0){
1149  if (!FlagPartialQFU){
1150  CHQ3_22 = value;
1151  }
1152  } else if (name.compare("CHQ3_23r") == 0)
1153  CHQ3_23r = value;
1154  else if (name.compare("CHQ3_33") == 0)
1155  CHQ3_33 = value;
1156  else if (name.compare("CHQ3_12i") == 0)
1157  CHQ3_12i = value;
1158  else if (name.compare("CHQ3_13i") == 0)
1159  CHQ3_13i = value;
1160  else if (name.compare("CHQ3_23i") == 0)
1161  CHQ3_23i = value;
1162  else if (name.compare("CHQ3") == 0) {
1163  CHQ3_11 = value;
1164  CHQ3_12r = 0.0;
1165  CHQ3_13r = 0.0;
1166  CHQ3_22 = value;
1167  CHQ3_23r = 0.0;
1168  CHQ3_33 = value;
1169  CHQ3_12i = 0.0;
1170  CHQ3_13i = 0.0;
1171  CHQ3_23i = 0.0;
1172  } else if (name.compare("CHu_11") == 0){
1173  CHu_11 = value;
1174  if (FlagPartialQFU){
1175  CHu_22 = value;
1176  }
1177  } else if (name.compare("CHu_12r") == 0)
1178  CHu_12r = value;
1179  else if (name.compare("CHu_13r") == 0)
1180  CHu_13r = value;
1181  else if (name.compare("CHu_22") == 0){
1182  if (!FlagPartialQFU){
1183  CHu_22 = value;
1184  }
1185  } else if (name.compare("CHu_23r") == 0)
1186  CHu_23r = value;
1187  else if (name.compare("CHu_33") == 0)
1188  CHu_33 = value;
1189  else if (name.compare("CHu_12i") == 0)
1190  CHu_12i = value;
1191  else if (name.compare("CHu_13i") == 0)
1192  CHu_13i = value;
1193  else if (name.compare("CHu_23i") == 0)
1194  CHu_23i = value;
1195  else if (name.compare("CHu") == 0) {
1196  CHu_11 = value;
1197  CHu_12r = 0.0;
1198  CHu_13r = 0.0;
1199  CHu_22 = value;
1200  CHu_23r = 0.0;
1201  CHu_33 = value;
1202  CHu_12i = 0.0;
1203  CHu_13i = 0.0;
1204  CHu_23i = 0.0;
1205  } else if (name.compare("CHd_11") == 0){
1206  CHd_11 = value;
1207  if (FlagPartialQFU){
1208  CHd_22 = value;
1209  }
1210  } else if (name.compare("CHd_12r") == 0)
1211  CHd_12r = value;
1212  else if (name.compare("CHd_13r") == 0)
1213  CHd_13r = value;
1214  else if (name.compare("CHd_22") == 0){
1215  if (!FlagPartialQFU){
1216  CHd_22 = value;
1217  }
1218  } else if (name.compare("CHd_23r") == 0)
1219  CHd_23r = value;
1220  else if (name.compare("CHd_33") == 0)
1221  CHd_33 = value;
1222  else if (name.compare("CHd_12i") == 0)
1223  CHd_12i = value;
1224  else if (name.compare("CHd_13i") == 0)
1225  CHd_13i = value;
1226  else if (name.compare("CHd_23i") == 0)
1227  CHd_23i = value;
1228  else if (name.compare("CHd") == 0) {
1229  CHd_11 = value;
1230  CHd_12r = 0.0;
1231  CHd_13r = 0.0;
1232  CHd_22 = value;
1233  CHd_23r = 0.0;
1234  CHd_33 = value;
1235  CHd_12i = 0.0;
1236  CHd_13i = 0.0;
1237  CHd_23i = 0.0;
1238  } else if (name.compare("CHud_11r") == 0){
1239  CHud_11r = value;
1240  if (FlagPartialQFU){
1241  CHud_22r = value;
1242  }
1243  } else if (name.compare("CHud_12r") == 0)
1244  CHud_12r = value;
1245  else if (name.compare("CHud_13r") == 0)
1246  CHud_13r = value;
1247  else if (name.compare("CHud_22r") == 0){
1248  if (!FlagPartialQFU){
1249  CHud_22r = value;
1250  }
1251  } else if (name.compare("CHud_23r") == 0)
1252  CHud_23r = value;
1253  else if (name.compare("CHud_33r") == 0)
1254  CHud_33r = value;
1255  else if (name.compare("CHud_r") == 0) {
1256  CHud_11r = value;
1257  CHud_12r = 0.0;
1258  CHud_13r = 0.0;
1259  CHud_22r = value;
1260  CHud_23r = 0.0;
1261  CHud_33r = value;
1262  } else if (name.compare("CHud_11i") == 0){
1263  CHud_11i = value;
1264  if (FlagPartialQFU){
1265  CHud_22i = value;
1266  }
1267  } else if (name.compare("CHud_12i") == 0)
1268  CHud_12i = value;
1269  else if (name.compare("CHud_13i") == 0)
1270  CHud_13i = value;
1271  else if (name.compare("CHud_22i") == 0){
1272  if (!FlagPartialQFU){
1273  CHud_22i = value;
1274  }
1275  } else if (name.compare("CHud_23i") == 0)
1276  CHud_23i = value;
1277  else if (name.compare("CHud_33i") == 0)
1278  CHud_33i = value;
1279  else if (name.compare("CHud_i") == 0) {
1280  CHud_11i = value;
1281  CHud_12i = 0.0;
1282  CHud_13i = 0.0;
1283  CHud_22i = value;
1284  CHud_23i = 0.0;
1285  CHud_33i = value;
1286  } else if (name.compare("CeH_11r") == 0){
1287  if (!FlagFlavU3OfX){
1288  CeH_11r = value;
1289  }
1290  } else if (name.compare("CeH_12r") == 0)
1291  CeH_12r = value;
1292  else if (name.compare("CeH_13r") == 0)
1293  CeH_13r = value;
1294  else if (name.compare("CeH_22r") == 0){
1295  if (!FlagFlavU3OfX){
1296  CeH_22r = value;
1297  }
1298  } else if (name.compare("CeH_23r") == 0)
1299  CeH_23r = value;
1300  else if (name.compare("CeH_33r") == 0){
1301  CeH_33r = value;
1302  if (FlagFlavU3OfX){
1303  CeH_11r = value;
1304  CeH_22r = value;
1305  }
1306  } else if (name.compare("CeH_11i") == 0)
1307  CeH_11i = value;
1308  else if (name.compare("CeH_12i") == 0)
1309  CeH_12i = value;
1310  else if (name.compare("CeH_13i") == 0)
1311  CeH_13i = value;
1312  else if (name.compare("CeH_22i") == 0)
1313  CeH_22i = value;
1314  else if (name.compare("CeH_23i") == 0)
1315  CeH_23i = value;
1316  else if (name.compare("CeH_33i") == 0)
1317  CeH_33i = value;
1318  else if (name.compare("CuH_11r") == 0){
1319  if (!FlagFlavU3OfX){
1320  CuH_11r = value;
1321  }
1322  } else if (name.compare("CuH_12r") == 0)
1323  CuH_12r = value;
1324  else if (name.compare("CuH_13r") == 0)
1325  CuH_13r = value;
1326  else if (name.compare("CuH_22r") == 0){
1327  if (!FlagFlavU3OfX){
1328  CuH_22r = value;
1329  }
1330  } else if (name.compare("CuH_23r") == 0)
1331  CuH_23r = value;
1332  else if (name.compare("CuH_33r") == 0){
1333  CuH_33r = value;
1334  if (FlagFlavU3OfX){
1335  CuH_11r = value;
1336  CuH_22r = value;
1337  }
1338  } else if (name.compare("CuH_11i") == 0)
1339  CuH_11i = value;
1340  else if (name.compare("CuH_12i") == 0)
1341  CuH_12i = value;
1342  else if (name.compare("CuH_13i") == 0)
1343  CuH_13i = value;
1344  else if (name.compare("CuH_22i") == 0)
1345  CuH_22i = value;
1346  else if (name.compare("CuH_23i") == 0)
1347  CuH_23i = value;
1348  else if (name.compare("CuH_33i") == 0)
1349  CuH_33i = value;
1350  else if (name.compare("CdH_11r") == 0){
1351  if (!FlagFlavU3OfX){
1352  CdH_11r = value;
1353  }
1354  } else if (name.compare("CdH_12r") == 0)
1355  CdH_12r = value;
1356  else if (name.compare("CdH_13r") == 0)
1357  CdH_13r = value;
1358  else if (name.compare("CdH_22r") == 0){
1359  if (!FlagFlavU3OfX){
1360  CdH_22r = value;
1361  }
1362  } else if (name.compare("CdH_23r") == 0)
1363  CdH_23r = value;
1364  else if (name.compare("CdH_33r") == 0){
1365  CdH_33r = value;
1366  if (FlagFlavU3OfX){
1367  CdH_11r = value;
1368  CdH_22r = value;
1369  }
1370  } else if (name.compare("CdH_11i") == 0)
1371  CdH_11i = value;
1372  else if (name.compare("CdH_12i") == 0)
1373  CdH_12i = value;
1374  else if (name.compare("CdH_13i") == 0)
1375  CdH_13i = value;
1376  else if (name.compare("CdH_22i") == 0)
1377  CdH_22i = value;
1378  else if (name.compare("CdH_23i") == 0)
1379  CdH_23i = value;
1380  else if (name.compare("CdH_33i") == 0)
1381  CdH_33i = value;
1382  else if (name.compare("CuG_11r") == 0){
1383  if (!FlagFlavU3OfX){
1384  CuG_11r = value;
1385  }
1386  } else if (name.compare("CuG_12r") == 0)
1387  CuG_12r = value;
1388  else if (name.compare("CuG_13r") == 0)
1389  CuG_13r = value;
1390  else if (name.compare("CuG_22r") == 0){
1391  if (!FlagFlavU3OfX){
1392  CuG_22r = value;
1393  }
1394  } else if (name.compare("CuG_23r") == 0)
1395  CuG_23r = value;
1396  else if (name.compare("CuG_33r") == 0){
1397  CuG_33r = value;
1398  if (FlagFlavU3OfX){
1399  CuG_11r = value;
1400  CuG_22r = value;
1401  }
1402  } else if (name.compare("CuG_r") == 0) {
1403  CuG_11r = value;
1404  CuG_12r = 0.0;
1405  CuG_13r = 0.0;
1406  CuG_22r = value;
1407  CuG_23r = 0.0;
1408  CuG_33r = value;
1409  } else if (name.compare("CuG_11i") == 0)
1410  CuG_11i = value;
1411  else if (name.compare("CuG_12i") == 0)
1412  CuG_12i = value;
1413  else if (name.compare("CuG_13i") == 0)
1414  CuG_13i = value;
1415  else if (name.compare("CuG_22i") == 0)
1416  CuG_22i = value;
1417  else if (name.compare("CuG_23i") == 0)
1418  CuG_23i = value;
1419  else if (name.compare("CuG_33i") == 0)
1420  CuG_33i = value;
1421  else if (name.compare("CuG_i") == 0) {
1422  CuG_11i = value;
1423  CuG_12i = 0.0;
1424  CuG_13i = 0.0;
1425  CuG_22i = value;
1426  CuG_23i = 0.0;
1427  CuG_33i = value;
1428  } else if (name.compare("CuW_11r") == 0){
1429  if (!FlagFlavU3OfX){
1430  CuW_11r = value;
1431  }
1432  } else if (name.compare("CuW_12r") == 0)
1433  CuW_12r = value;
1434  else if (name.compare("CuW_13r") == 0)
1435  CuW_13r = value;
1436  else if (name.compare("CuW_22r") == 0){
1437  if (!FlagFlavU3OfX){
1438  CuW_22r = value;
1439  }
1440  } else if (name.compare("CuW_23r") == 0)
1441  CuW_23r = value;
1442  else if (name.compare("CuW_33r") == 0){
1443  CuW_33r = value;
1444  if (FlagFlavU3OfX){
1445  CuW_11r = value;
1446  CuW_22r = value;
1447  }
1448  } else if (name.compare("CuW_r") == 0) {
1449  CuW_11r = value;
1450  CuW_12r = 0.0;
1451  CuW_13r = 0.0;
1452  CuW_22r = value;
1453  CuW_23r = 0.0;
1454  CuW_33r = value;
1455  } else if (name.compare("CuW_11i") == 0)
1456  CuW_11i = value;
1457  else if (name.compare("CuW_12i") == 0)
1458  CuW_12i = value;
1459  else if (name.compare("CuW_13i") == 0)
1460  CuW_13i = value;
1461  else if (name.compare("CuW_22i") == 0)
1462  CuW_22i = value;
1463  else if (name.compare("CuW_23i") == 0)
1464  CuW_23i = value;
1465  else if (name.compare("CuW_33i") == 0)
1466  CuW_33i = value;
1467  else if (name.compare("CuW_i") == 0) {
1468  CuW_11i = value;
1469  CuW_12i = 0.0;
1470  CuW_13i = 0.0;
1471  CuW_22i = value;
1472  CuW_23i = 0.0;
1473  CuW_33i = value;
1474  } else if (name.compare("CuB_11r") == 0){
1475  if (!FlagFlavU3OfX){
1476  CuB_11r = value;
1477  }
1478  } else if (name.compare("CuB_12r") == 0)
1479  CuB_12r = value;
1480  else if (name.compare("CuB_13r") == 0)
1481  CuB_13r = value;
1482  else if (name.compare("CuB_22r") == 0){
1483  if (!FlagFlavU3OfX){
1484  CuB_22r = value;
1485  }
1486  } else if (name.compare("CuB_23r") == 0)
1487  CuB_23r = value;
1488  else if (name.compare("CuB_33r") == 0){
1489  CuB_33r = value;
1490  if (FlagFlavU3OfX){
1491  CuB_11r = value;
1492  CuB_22r = value;
1493  }
1494  } else if (name.compare("CuB_r") == 0) {
1495  CuB_11r = value;
1496  CuB_12r = 0.0;
1497  CuB_13r = 0.0;
1498  CuB_22r = value;
1499  CuB_23r = 0.0;
1500  CuB_33r = value;
1501  } else if (name.compare("CuB_11i") == 0)
1502  CuB_11i = value;
1503  else if (name.compare("CuB_12i") == 0)
1504  CuB_12i = value;
1505  else if (name.compare("CuB_13i") == 0)
1506  CuB_13i = value;
1507  else if (name.compare("CuB_22i") == 0)
1508  CuB_22i = value;
1509  else if (name.compare("CuB_23i") == 0)
1510  CuB_23i = value;
1511  else if (name.compare("CuB_33i") == 0)
1512  CuB_33i = value;
1513  else if (name.compare("CuB_i") == 0) {
1514  CuB_11i = value;
1515  CuB_12i = 0.0;
1516  CuB_13i = 0.0;
1517  CuB_22i = value;
1518  CuB_23i = 0.0;
1519  CuB_33i = value;
1520 // Several redundancies for the 4-fermionn operators below
1521  } else if (name.compare("CLL_1111") == 0) {
1522  CLL_1111 = value;
1523  } else if (name.compare("CLL_1122") == 0) {
1524  CLL_1122 = value;
1525  CLL_2211 = value;
1526  } else if (name.compare("CLL_1133") == 0) {
1527  CLL_1133 = value;
1528  CLL_3311 = value;
1529  } else if (name.compare("CLL_1221") == 0) {
1530  CLL_1221 = value;
1531  CLL_2112 = value;
1532  } else if (name.compare("CLL_1331") == 0) {
1533  CLL_1331 = value;
1534  CLL_3113 = value;
1535  } else if (name.compare("CLL") == 0) {
1536  CLL_1111 = value;
1537  CLL_1221 = value;
1538  CLL_2112 = value;
1539  CLL_2211 = value;
1540  CLL_1122 = value;
1541  CLL_3311 = value;
1542  CLL_1133 = value;
1543  CLL_1331 = value;
1544  CLL_3113 = value;
1545  } else if (name.compare("CLQ1_1111") == 0) {
1546  CLQ1_1111 = value;
1547  } else if (name.compare("CLQ1_1122") == 0) {
1548  CLQ1_1122 = value;
1549  } else if (name.compare("CLQ1_2211") == 0) {
1550  CLQ1_2211 = value;
1551  } else if (name.compare("CLQ1_2112") == 0) {
1552  CLQ1_2112 = value;
1553  } else if (name.compare("CLQ1_1221") == 0) {
1554  CLQ1_1221 = value;
1555  } else if (name.compare("CLQ1_1133") == 0) {
1556  CLQ1_1133 = value;
1557  } else if (name.compare("CLQ1_3311") == 0) {
1558  CLQ1_3311 = value;
1559  } else if (name.compare("CLQ1_3113") == 0) {
1560  CLQ1_3113 = value;
1561  } else if (name.compare("CLQ1_1331") == 0) {
1562  CLQ1_1331 = value;
1563  } else if (name.compare("CLQ1_1123") == 0) {
1564  CLQ1_1123 = value;
1565  } else if (name.compare("CLQ1_2223") == 0) {
1566  CLQ1_2223 = value;
1567  } else if (name.compare("CLQ1_3323") == 0) {
1568  CLQ1_3323 = value;
1569  } else if (name.compare("CLQ1_1132") == 0) {
1570  CLQ1_1132 = value;
1571  } else if (name.compare("CLQ1_2232") == 0) {
1572  CLQ1_2232 = value;
1573  } else if (name.compare("CLQ1_3332") == 0) {
1574  CLQ1_3332 = value;
1575  } else if (name.compare("CLQ1") == 0) {
1576  CLQ1_1111 = value;
1577  CLQ1_1122 = value;
1578  CLQ1_2211 = value;
1579  CLQ1_1221 = value;
1580  CLQ1_2112 = value;
1581  CLQ1_1133 = value;
1582  CLQ1_3311 = value;
1583  CLQ1_1331 = value;
1584  CLQ1_3113 = value;
1585  } else if (name.compare("CLQ3_1111") == 0) {
1586  CLQ3_1111 = value;
1587  } else if (name.compare("CLQ3_1122") == 0) {
1588  CLQ3_1122 = value;
1589  } else if (name.compare("CLQ3_2211") == 0) {
1590  CLQ3_2211 = value;
1591  } else if (name.compare("CLQ3_2112") == 0) {
1592  CLQ3_2112 = value;
1593  } else if (name.compare("CLQ3_1221") == 0) {
1594  CLQ3_1221 = value;
1595  } else if (name.compare("CLQ3_1133") == 0) {
1596  CLQ3_1133 = value;
1597  } else if (name.compare("CLQ3_3311") == 0) {
1598  CLQ3_3311 = value;
1599  } else if (name.compare("CLQ3_3113") == 0) {
1600  CLQ3_3113 = value;
1601  } else if (name.compare("CLQ3_1331") == 0) {
1602  CLQ3_1331 = value;
1603  } else if (name.compare("CLQ3_1123") == 0) {
1604  CLQ3_1123 = value;
1605  } else if (name.compare("CLQ3_2223") == 0) {
1606  CLQ3_2223 = value;
1607  } else if (name.compare("CLQ3_3323") == 0) {
1608  CLQ3_3323 = value;
1609  } else if (name.compare("CLQ3_1132") == 0) {
1610  CLQ3_1132 = value;
1611  } else if (name.compare("CLQ3_2232") == 0) {
1612  CLQ3_2232 = value;
1613  } else if (name.compare("CLQ3_3332") == 0) {
1614  CLQ3_3332 = value;
1615  } else if (name.compare("CLQ3") == 0) {
1616  CLQ3_1111 = value;
1617  CLQ3_1122 = value;
1618  CLQ3_2211 = value;
1619  CLQ3_1221 = value;
1620  CLQ3_2112 = value;
1621  CLQ3_1133 = value;
1622  CLQ3_3311 = value;
1623  CLQ3_1331 = value;
1624  CLQ3_3113 = value;
1625  } else if (name.compare("Cee") == 0) {
1626  Cee_1111 = value;
1627  Cee_1122 = value;
1628  Cee_2211 = value;
1629  Cee_1133 = value;
1630  Cee_3311 = value;
1631  } else if (name.compare("Cee_1111") == 0) {
1632  Cee_1111 = value;
1633  } else if (name.compare("Cee_1122") == 0) {
1634  Cee_1122 = value;
1635  Cee_2211 = value;
1636  } else if (name.compare("Cee_1133") == 0) {
1637  Cee_1133 = value;
1638  Cee_3311 = value;
1639  } else if (name.compare("Ceu") == 0) {
1640  Ceu_1111 = value;
1641  Ceu_1122 = value;
1642  Ceu_2211 = value;
1643  Ceu_1133 = value;
1644  Ceu_2233 = value;
1645  Ceu_3311 = value;
1646  } else if (name.compare("Ceu_1111") == 0) {
1647  Ceu_1111 = value;
1648  } else if (name.compare("Ceu_1122") == 0) {
1649  Ceu_1122 = value;
1650  } else if (name.compare("Ceu_2211") == 0) {
1651  Ceu_2211 = value;
1652  } else if (name.compare("Ceu_1133") == 0) {
1653  Ceu_1133 = value;
1654  } else if (name.compare("Ceu_2233") == 0) {
1655  Ceu_2233 = value;
1656  } else if (name.compare("Ceu_3311") == 0) {
1657  Ceu_3311 = value;
1658  } else if (name.compare("Ced") == 0) {
1659  Ced_1111 = value;
1660  Ced_1122 = value;
1661  Ced_2211 = value;
1662  Ced_1133 = value;
1663  Ced_3311 = value;
1664  } else if (name.compare("Ced_1111") == 0) {
1665  Ced_1111 = value;
1666  } else if (name.compare("Ced_1122") == 0) {
1667  Ced_1122 = value;
1668  } else if (name.compare("Ced_2211") == 0) {
1669  Ced_2211 = value;
1670  } else if (name.compare("Ced_1133") == 0) {
1671  Ced_1133 = value;
1672  } else if (name.compare("Ced_3311") == 0) {
1673  Ced_3311 = value;
1674  } else if (name.compare("Ced_1123") == 0) {
1675  Ced_1123 = value;
1676  } else if (name.compare("Ced_2223") == 0) {
1677  Ced_2223 = value;
1678  } else if (name.compare("Ced_3323") == 0) {
1679  Ced_3323 = value;
1680  } else if (name.compare("Ced_1132") == 0) {
1681  Ced_1132 = value;
1682  } else if (name.compare("Ced_2232") == 0) {
1683  Ced_2232 = value;
1684  } else if (name.compare("Ced_3332") == 0) {
1685  Ced_3332 = value;
1686  } else if (name.compare("CLe") == 0) {
1687  CLe_1111 = value;
1688  CLe_1122 = value;
1689  CLe_2211 = value;
1690  CLe_1133 = value;
1691  CLe_3311 = value;
1692  } else if (name.compare("CLe_1111") == 0) {
1693  CLe_1111 = value;
1694  } else if (name.compare("CLe_1122") == 0) {
1695  CLe_1122 = value;
1696  } else if (name.compare("CLe_2211") == 0) {
1697  CLe_2211 = value;
1698  } else if (name.compare("CLe_1133") == 0) {
1699  CLe_1133 = value;
1700  } else if (name.compare("CLe_3311") == 0) {
1701  CLe_3311 = value;
1702  } else if (name.compare("CLu") == 0) {
1703  CLu_1111 = value;
1704  CLu_1122 = value;
1705  CLu_2211 = value;
1706  CLu_1133 = value;
1707  CLu_2233 = value;
1708  CLu_3311 = value;
1709  } else if (name.compare("CLu_1111") == 0) {
1710  CLu_1111 = value;
1711  } else if (name.compare("CLu_1122") == 0) {
1712  CLu_1122 = value;
1713  } else if (name.compare("CLu_2211") == 0) {
1714  CLu_2211 = value;
1715  } else if (name.compare("CLu_1133") == 0) {
1716  CLu_1133 = value;
1717  } else if (name.compare("CLu_2233") == 0) {
1718  CLu_2233 = value;
1719  } else if (name.compare("CLu_3311") == 0) {
1720  CLu_3311 = value;
1721  } else if (name.compare("CLd") == 0) {
1722  CLd_1111 = value;
1723  CLd_1122 = value;
1724  CLd_2211 = value;
1725  CLd_1133 = value;
1726  CLd_3311 = value;
1727  } else if (name.compare("CLd_1111") == 0) {
1728  CLd_1111 = value;
1729  } else if (name.compare("CLd_1122") == 0) {
1730  CLd_1122 = value;
1731  } else if (name.compare("CLd_2211") == 0) {
1732  CLd_2211 = value;
1733  } else if (name.compare("CLd_1133") == 0) {
1734  CLd_1133 = value;
1735  } else if (name.compare("CLd_3311") == 0) {
1736  CLd_3311 = value;
1737  } else if (name.compare("CLd_1123") == 0) {
1738  CLd_1123 = value;
1739  } else if (name.compare("CLd_2223") == 0) {
1740  CLd_2223 = value;
1741  } else if (name.compare("CLd_3323") == 0) {
1742  CLd_3323 = value;
1743  } else if (name.compare("CLd_1132") == 0) {
1744  CLd_1132 = value;
1745  } else if (name.compare("CLd_2232") == 0) {
1746  CLd_2232 = value;
1747  } else if (name.compare("CLd_3332") == 0) {
1748  CLd_3332 = value;
1749  } else if (name.compare("CQe") == 0) {
1750  CQe_1111 = value;
1751  CQe_1122 = value;
1752  CQe_2211 = value;
1753  CQe_1133 = value;
1754  CQe_3311 = value;
1755  } else if (name.compare("CQe_1111") == 0) {
1756  CQe_1111 = value;
1757  } else if (name.compare("CQe_1122") == 0) {
1758  CQe_1122 = value;
1759  } else if (name.compare("CQe_2211") == 0) {
1760  CQe_2211 = value;
1761  } else if (name.compare("CQe_1133") == 0) {
1762  CQe_1133 = value;
1763  } else if (name.compare("CQe_3311") == 0) {
1764  CQe_3311 = value;
1765  } else if (name.compare("CQe_2311") == 0) {
1766  CQe_2311 = value;
1767  } else if (name.compare("CQe_2322") == 0) {
1768  CQe_2322 = value;
1769  } else if (name.compare("CQe_2333") == 0) {
1770  CQe_2333 = value;
1771  } else if (name.compare("CQe_3211") == 0) {
1772  CQe_3211 = value;
1773  } else if (name.compare("CQe_3222") == 0) {
1774  CQe_3222 = value;
1775  } else if (name.compare("CLedQ_11") == 0) {
1776  CLedQ_11 = value;
1777  } else if (name.compare("CLedQ_22") == 0) {
1778  CLedQ_22 = value;
1779  } else if (name.compare("CpLedQ_11") == 0) {
1780  CpLedQ_11 = value;
1781  } else if (name.compare("CpLedQ_22") == 0) {
1782  CpLedQ_22 = value;
1783  } else if (name.compare("CQe_3233") == 0) {
1784  CQe_3233 = value;
1785  } else if (name.compare("Lambda_NP") == 0) {
1786  Lambda_NP = value;
1787  } else if (name.compare("BrHinv") == 0) {
1788 // Always positive
1789  BrHinv = fabs(value);
1790  } else if (name.compare("BrHexo") == 0) {
1791 // Always positive
1792  BrHexo = fabs(value);
1793  } else if (name.compare("dg1Z") == 0) {
1794  dg1Z = value;
1795  } else if (name.compare("dKappaga") == 0) {
1796  dKappaga = value;
1797  } else if (name.compare("lambZ") == 0) {
1798  lambZ = value;
1799  } else if (name.compare("eggFint") == 0) {
1800  eggFint = value;
1801  } else if (name.compare("eggFpar") == 0) {
1802  eggFpar = value;
1803  } else if (name.compare("ettHint") == 0) {
1804  ettHint = value;
1805  } else if (name.compare("ettHpar") == 0) {
1806  ettHpar = value;
1807  } else if (name.compare("eVBFint") == 0) {
1808  eVBFint = value;
1809  } else if (name.compare("eVBFpar") == 0) {
1810  eVBFpar = value;
1811  } else if (name.compare("eWHint") == 0) {
1812  eWHint = value;
1813  } else if (name.compare("eWHpar") == 0) {
1814  eWHpar = value;
1815  } else if (name.compare("eZHint") == 0) {
1816  eZHint = value;
1817  } else if (name.compare("eZHpar") == 0) {
1818  eZHpar = value;
1819  } else if (name.compare("eeeWBFint") == 0) {
1820  eeeWBFint = value;
1821  } else if (name.compare("eeeWBFpar") == 0) {
1822  eeeWBFpar = value;
1823  } else if (name.compare("eeeZHint") == 0) {
1824  eeeZHint = value;
1825  } else if (name.compare("eeeZHpar") == 0) {
1826  eeeZHpar = value;
1827  } else if (name.compare("eeettHint") == 0) {
1828  eeettHint = value;
1829  } else if (name.compare("eeettHpar") == 0) {
1830  eeettHpar = value;
1831  } else if (name.compare("eHggint") == 0) {
1832  eHggint = value;
1833  } else if (name.compare("eHggpar") == 0) {
1834  eHggpar = value;
1835  } else if (name.compare("eHWWint") == 0) {
1836  eHWWint = value;
1837  } else if (name.compare("eHWWpar") == 0) {
1838  eHWWpar = value;
1839  } else if (name.compare("eHZZint") == 0) {
1840  eHZZint = value;
1841  } else if (name.compare("eHZZpar") == 0) {
1842  eHZZpar = value;
1843  } else if (name.compare("eHZgaint") == 0) {
1844  eHZgaint = value;
1845  } else if (name.compare("eHZgapar") == 0) {
1846  eHZgapar = value;
1847  } else if (name.compare("eHgagaint") == 0) {
1848  eHgagaint = value;
1849  } else if (name.compare("eHgagapar") == 0) {
1850  eHgagapar = value;
1851  } else if (name.compare("eHmumuint") == 0) {
1852  eHmumuint = value;
1853  } else if (name.compare("eHmumupar") == 0) {
1854  eHmumupar = value;
1855  } else if (name.compare("eHtautauint") == 0) {
1856  eHtautauint = value;
1857  } else if (name.compare("eHtautaupar") == 0) {
1858  eHtautaupar = value;
1859  } else if (name.compare("eHccint") == 0) {
1860  eHccint = value;
1861  } else if (name.compare("eHccpar") == 0) {
1862  eHccpar = value;
1863  } else if (name.compare("eHbbint") == 0) {
1864  eHbbint = value;
1865  } else if (name.compare("eHbbpar") == 0) {
1866  eHbbpar = value;
1867  } else if (name.compare("eVBF_2_Hbox") == 0) {
1868  eVBF_2_Hbox = value;
1869  } else if (name.compare("eVBF_2_HQ1_11") == 0) {
1870  eVBF_2_HQ1_11 = value;
1871  } else if (name.compare("eVBF_2_Hu_11") == 0) {
1872  eVBF_2_Hu_11 = value;
1873  } else if (name.compare("eVBF_2_Hd_11") == 0) {
1874  eVBF_2_Hd_11 = value;
1875  } else if (name.compare("eVBF_2_HQ3_11") == 0) {
1876  eVBF_2_HQ3_11 = value;
1877  } else if (name.compare("eVBF_2_HD") == 0) {
1878  eVBF_2_HD = value;
1879  } else if (name.compare("eVBF_2_HB") == 0) {
1880  eVBF_2_HB = value;
1881  } else if (name.compare("eVBF_2_HW") == 0) {
1882  eVBF_2_HW = value;
1883  } else if (name.compare("eVBF_2_HWB") == 0) {
1884  eVBF_2_HWB = value;
1885  } else if (name.compare("eVBF_2_HG") == 0) {
1886  eVBF_2_HG = value;
1887  } else if (name.compare("eVBF_2_DHB") == 0) {
1888  eVBF_2_DHB = value;
1889  } else if (name.compare("eVBF_2_DHW") == 0) {
1890  eVBF_2_DHW = value;
1891  } else if (name.compare("eVBF_2_DeltaGF") == 0) {
1892  eVBF_2_DeltaGF = value;
1893  } else if (name.compare("eVBF_78_Hbox") == 0) {
1894  eVBF_78_Hbox = value;
1895  } else if (name.compare("eVBF_78_HQ1_11") == 0) {
1896  eVBF_78_HQ1_11 = value;
1897  } else if (name.compare("eVBF_78_Hu_11") == 0) {
1898  eVBF_78_Hu_11 = value;
1899  } else if (name.compare("eVBF_78_Hd_11") == 0) {
1900  eVBF_78_Hd_11 = value;
1901  } else if (name.compare("eVBF_78_HQ3_11") == 0) {
1902  eVBF_78_HQ3_11 = value;
1903  } else if (name.compare("eVBF_78_HD") == 0) {
1904  eVBF_78_HD = value;
1905  } else if (name.compare("eVBF_78_HB") == 0) {
1906  eVBF_78_HB = value;
1907  } else if (name.compare("eVBF_78_HW") == 0) {
1908  eVBF_78_HW = value;
1909  } else if (name.compare("eVBF_78_HWB") == 0) {
1910  eVBF_78_HWB = value;
1911  } else if (name.compare("eVBF_78_HG") == 0) {
1912  eVBF_78_HG = value;
1913  } else if (name.compare("eVBF_78_DHB") == 0) {
1914  eVBF_78_DHB = value;
1915  } else if (name.compare("eVBF_78_DHW") == 0) {
1916  eVBF_78_DHW = value;
1917  } else if (name.compare("eVBF_78_DeltaGF") == 0) {
1918  eVBF_78_DeltaGF = value;
1919  } else if (name.compare("eVBF_1314_Hbox") == 0) {
1920  eVBF_1314_Hbox = value;
1921  } else if (name.compare("eVBF_1314_HQ1_11") == 0) {
1922  eVBF_1314_HQ1_11 = value;
1923  } else if (name.compare("eVBF_1314_Hu_11") == 0) {
1924  eVBF_1314_Hu_11 = value;
1925  } else if (name.compare("eVBF_1314_Hd_11") == 0) {
1926  eVBF_1314_Hd_11 = value;
1927  } else if (name.compare("eVBF_1314_HQ3_11") == 0) {
1928  eVBF_1314_HQ3_11 = value;
1929  } else if (name.compare("eVBF_1314_HD") == 0) {
1930  eVBF_1314_HD = value;
1931  } else if (name.compare("eVBF_1314_HB") == 0) {
1932  eVBF_1314_HB = value;
1933  } else if (name.compare("eVBF_1314_HW") == 0) {
1934  eVBF_1314_HW = value;
1935  } else if (name.compare("eVBF_1314_HWB") == 0) {
1936  eVBF_1314_HWB = value;
1937  } else if (name.compare("eVBF_1314_HG") == 0) {
1938  eVBF_1314_HG = value;
1939  } else if (name.compare("eVBF_1314_DHB") == 0) {
1940  eVBF_1314_DHB = value;
1941  } else if (name.compare("eVBF_1314_DHW") == 0) {
1942  eVBF_1314_DHW = value;
1943  } else if (name.compare("eVBF_1314_DeltaGF") == 0) {
1944  eVBF_1314_DeltaGF = value;
1945  } else if (name.compare("eWH_2_Hbox") == 0) {
1946  eWH_2_Hbox = value;
1947  } else if (name.compare("eWH_2_HQ3_11") == 0) {
1948  eWH_2_HQ3_11 = value;
1949  } else if (name.compare("eWH_2_HD") == 0) {
1950  eWH_2_HD = value;
1951  } else if (name.compare("eWH_2_HW") == 0) {
1952  eWH_2_HW = value;
1953  } else if (name.compare("eWH_2_HWB") == 0) {
1954  eWH_2_HWB = value;
1955  } else if (name.compare("eWH_2_DHW") == 0) {
1956  eWH_2_DHW = value;
1957  } else if (name.compare("eWH_2_DeltaGF") == 0) {
1958  eWH_2_DeltaGF = value;
1959  } else if (name.compare("eWH_78_Hbox") == 0) {
1960  eWH_78_Hbox = value;
1961  } else if (name.compare("eWH_78_HQ3_11") == 0) {
1962  eWH_78_HQ3_11 = value;
1963  } else if (name.compare("eWH_78_HD") == 0) {
1964  eWH_78_HD = value;
1965  } else if (name.compare("eWH_78_HW") == 0) {
1966  eWH_78_HW = value;
1967  } else if (name.compare("eWH_78_HWB") == 0) {
1968  eWH_78_HWB = value;
1969  } else if (name.compare("eWH_78_DHW") == 0) {
1970  eWH_78_DHW = value;
1971  } else if (name.compare("eWH_78_DeltaGF") == 0) {
1972  eWH_78_DeltaGF = value;
1973  } else if (name.compare("eWH_1314_Hbox") == 0) {
1974  eWH_1314_Hbox = value;
1975  } else if (name.compare("eWH_1314_HQ3_11") == 0) {
1976  eWH_1314_HQ3_11 = value;
1977  } else if (name.compare("eWH_1314_HD") == 0) {
1978  eWH_1314_HD = value;
1979  } else if (name.compare("eWH_1314_HW") == 0) {
1980  eWH_1314_HW = value;
1981  } else if (name.compare("eWH_1314_HWB") == 0) {
1982  eWH_1314_HWB = value;
1983  } else if (name.compare("eWH_1314_DHW") == 0) {
1984  eWH_1314_DHW = value;
1985  } else if (name.compare("eWH_1314_DeltaGF") == 0) {
1986  eWH_1314_DeltaGF = value;
1987  } else if (name.compare("eZH_2_Hbox") == 0) {
1988  eZH_2_Hbox = value;
1989  } else if (name.compare("eZH_2_HQ1_11") == 0) {
1990  eZH_2_HQ1_11 = value;
1991  } else if (name.compare("eZH_2_Hu_11") == 0) {
1992  eZH_2_Hu_11 = value;
1993  } else if (name.compare("eZH_2_Hd_11") == 0) {
1994  eZH_2_Hd_11 = value;
1995  } else if (name.compare("eZH_2_HQ3_11") == 0) {
1996  eZH_2_HQ3_11 = value;
1997  } else if (name.compare("eZH_2_HD") == 0) {
1998  eZH_2_HD = value;
1999  } else if (name.compare("eZH_2_HB") == 0) {
2000  eZH_2_HB = value;
2001  } else if (name.compare("eZH_2_HW") == 0) {
2002  eZH_2_HW = value;
2003  } else if (name.compare("eZH_2_HWB") == 0) {
2004  eZH_2_HWB = value;
2005  } else if (name.compare("eZH_2_DHB") == 0) {
2006  eZH_2_DHB = value;
2007  } else if (name.compare("eZH_2_DHW") == 0) {
2008  eZH_2_DHW = value;
2009  } else if (name.compare("eZH_2_DeltaGF") == 0) {
2010  eZH_2_DeltaGF = value;
2011  } else if (name.compare("eZH_78_Hbox") == 0) {
2012  eZH_78_Hbox = value;
2013  } else if (name.compare("eZH_78_HQ1_11") == 0) {
2014  eZH_78_HQ1_11 = value;
2015  } else if (name.compare("eZH_78_Hu_11") == 0) {
2016  eZH_78_Hu_11 = value;
2017  } else if (name.compare("eZH_78_Hd_11") == 0) {
2018  eZH_78_Hd_11 = value;
2019  } else if (name.compare("eZH_78_HQ3_11") == 0) {
2020  eZH_78_HQ3_11 = value;
2021  } else if (name.compare("eZH_78_HD") == 0) {
2022  eZH_78_HD = value;
2023  } else if (name.compare("eZH_78_HB") == 0) {
2024  eZH_78_HB = value;
2025  } else if (name.compare("eZH_78_HW") == 0) {
2026  eZH_78_HW = value;
2027  } else if (name.compare("eZH_78_HWB") == 0) {
2028  eZH_78_HWB = value;
2029  } else if (name.compare("eZH_78_DHB") == 0) {
2030  eZH_78_DHB = value;
2031  } else if (name.compare("eZH_78_DHW") == 0) {
2032  eZH_78_DHW = value;
2033  } else if (name.compare("eZH_78_DeltaGF") == 0) {
2034  eZH_78_DeltaGF = value;
2035  } else if (name.compare("eZH_1314_Hbox") == 0) {
2036  eZH_1314_Hbox = value;
2037  } else if (name.compare("eZH_1314_HQ1_11") == 0) {
2038  eZH_1314_HQ1_11 = value;
2039  } else if (name.compare("eZH_1314_Hu_11") == 0) {
2040  eZH_1314_Hu_11 = value;
2041  } else if (name.compare("eZH_1314_Hd_11") == 0) {
2042  eZH_1314_Hd_11 = value;
2043  } else if (name.compare("eZH_1314_HQ3_11") == 0) {
2044  eZH_1314_HQ3_11 = value;
2045  } else if (name.compare("eZH_1314_HD") == 0) {
2046  eZH_1314_HD = value;
2047  } else if (name.compare("eZH_1314_HB") == 0) {
2048  eZH_1314_HB = value;
2049  } else if (name.compare("eZH_1314_HW") == 0) {
2050  eZH_1314_HW = value;
2051  } else if (name.compare("eZH_1314_HWB") == 0) {
2052  eZH_1314_HWB = value;
2053  } else if (name.compare("eZH_1314_DHB") == 0) {
2054  eZH_1314_DHB = value;
2055  } else if (name.compare("eZH_1314_DHW") == 0) {
2056  eZH_1314_DHW = value;
2057  } else if (name.compare("eZH_1314_DeltaGF") == 0) {
2058  eZH_1314_DeltaGF = value;
2059  } else if (name.compare("ettH_2_HG") == 0) {
2060  ettH_2_HG = value;
2061  } else if (name.compare("ettH_2_G") == 0) {
2062  ettH_2_G = value;
2063  } else if (name.compare("ettH_2_uG_33r") == 0) {
2064  ettH_2_uG_33r = value;
2065  } else if (name.compare("ettH_2_DeltagHt") == 0) {
2066  ettH_2_DeltagHt = value;
2067  } else if (name.compare("ettH_78_HG") == 0) {
2068  ettH_78_HG = value;
2069  } else if (name.compare("ettH_78_G") == 0) {
2070  ettH_78_G = value;
2071  } else if (name.compare("ettH_78_uG_33r") == 0) {
2072  ettH_78_uG_33r = value;
2073  } else if (name.compare("ettH_78_DeltagHt") == 0) {
2074  ettH_78_DeltagHt = value;
2075  } else if (name.compare("ettH_1314_HG") == 0) {
2076  ettH_1314_HG = value;
2077  } else if (name.compare("ettH_1314_G") == 0) {
2078  ettH_1314_G = value;
2079  } else if (name.compare("ettH_1314_uG_33r") == 0) {
2080  ettH_1314_uG_33r = value;
2081  } else if (name.compare("ettH_1314_DeltagHt") == 0) {
2082  ettH_1314_DeltagHt = value;
2083  } else
2084  NPbase::setParameter(name, value);
2085 }
double Ceu_1122
Definition: NPSMEFTd6.h:3608
double CQe_2322
Definition: NPSMEFTd6.h:3631
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3552
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3542
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3429
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3522
double CpLedQ_22
Definition: NPSMEFTd6.h:3633
double CLL_1111
Definition: NPSMEFTd6.h:3591
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3528
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3433
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3464
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3456
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3540
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3492
double eVBF_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3681
double eVBF_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3694
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3536
double eVBF_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3709
double eZH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3774
double CuG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3563
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3554
double eZH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3760
double CLe_1111
Definition: NPSMEFTd6.h:3616
double eZH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3763
double eHbbpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3669
double CLQ3_1111
Definition: NPSMEFTd6.h:3599
double eHtautauint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3664
double ettH_2_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3778
double eWH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3734
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3480
double eZH_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3738
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3453
double eZH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3737
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3521
double CQe_2211
Definition: NPSMEFTd6.h:3629
double eZH_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3756
double CLL_1221
Definition: NPSMEFTd6.h:3592
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3501
double eZH_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3766
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3482
double eZH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3742
double eVBF_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3706
double CLQ1_3323
Definition: NPSMEFTd6.h:3597
double CLd_1133
Definition: NPSMEFTd6.h:3625
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3590
double eZH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3748
double eWH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3721
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3494
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3508
double CuB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3587
double eVBF_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3703
double eVBF_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3707
double eWHpar
Parametric relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3643
double Cee_3311
Definition: NPSMEFTd6.h:3606
double eZH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3768
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3544
double Ced_1111
Definition: NPSMEFTd6.h:3611
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3550
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3567
double ettHpar
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3639
double eggFpar
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3637
double eVBF_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3695
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3538
double eZH_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3759
double eHtautaupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3665
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3543
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3435
double eVBF_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3685
double CLQ3_3323
Definition: NPSMEFTd6.h:3602
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3469
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3463
double CLL_1331
Definition: NPSMEFTd6.h:3593
double CH
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3443
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3515
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3549
double CLQ3_2223
Definition: NPSMEFTd6.h:3602
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3461
double Cee_1133
Definition: NPSMEFTd6.h:3606
double Ced_2232
Definition: NPSMEFTd6.h:3615
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3579
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3442
double CLQ3_2112
Definition: NPSMEFTd6.h:3600
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3640
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3474
double eVBF_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3687
double Ceu_2233
Definition: NPSMEFTd6.h:3610
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3441
double CuW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3571
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3511
double eWH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3714
double eZH_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3753
double CLL_2211
Definition: NPSMEFTd6.h:3592
double eVBF_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3672
double eVBF_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3674
double eVBF_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3671
double CuW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3577
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3447
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3654
double eVBF_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3673
double CuB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3586
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3481
double Ced_1132
Definition: NPSMEFTd6.h:3615
double CLu_1133
Definition: NPSMEFTd6.h:3621
double CLQ1_2112
Definition: NPSMEFTd6.h:3595
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3477
double eZH_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3743
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3506
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3510
double CHWHB_gagaorth
The combination of dimension-6 operator coefficients .
Definition: NPSMEFTd6.h:3437
double ettH_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3776
double CLQ3_1122
Definition: NPSMEFTd6.h:3600
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3555
double eHmumuint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3662
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3647
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3649
double eZH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3773
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3650
double eVBF_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3683
double CLQ3_2232
Definition: NPSMEFTd6.h:3603
double eVBF_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3686
double eZH_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3764
double eVBF_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3700
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3585
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3535
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3547
double eVBF_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3689
double dg1Z
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3796
double CLL_1133
Definition: NPSMEFTd6.h:3593
double eHgagaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3660
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3529
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3641
double eZH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3758
double ettH_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3781
double eVBF_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3701
double CLd_1123
Definition: NPSMEFTd6.h:3626
double CuB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3589
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3512
double eWH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3718
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3493
double eZH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3747
std::string name
The name of the model.
Definition: Model.h:246
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3468
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3438
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3514
double Ced_3323
Definition: NPSMEFTd6.h:3614
double eWH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3723
double eWH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3716
double eVBF_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3696
double CLQ3_1123
Definition: NPSMEFTd6.h:3602
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3798
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3656
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3657
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3566
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3452
double eHggpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3653
double eWH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3724
double eVBF_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3691
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3655
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3473
double CLQ1_1133
Definition: NPSMEFTd6.h:3596
double Ced_1123
Definition: NPSMEFTd6.h:3614
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3553
double CLe_3311
Definition: NPSMEFTd6.h:3618
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3519
double ettH_1314_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3787
double CLQ1_1123
Definition: NPSMEFTd6.h:3597
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3489
double C2B
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3431
double CLd_2223
Definition: NPSMEFTd6.h:3626
double CLQ1_3311
Definition: NPSMEFTd6.h:3596
double eHZgaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3658
double eHbbint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3668
double eWH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3725
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3558
double CLedQ_22
Definition: NPSMEFTd6.h:3633
double ettH_2_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3777
double CLQ1_2211
Definition: NPSMEFTd6.h:3595
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3485
double CLd_1111
Definition: NPSMEFTd6.h:3623
double eVBF_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3676
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3518
double CLQ1_1111
Definition: NPSMEFTd6.h:3594
double Ced_1133
Definition: NPSMEFTd6.h:3613
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3570
double eWH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3722
double eHZgapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3659
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3462
double C2W
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3432
double Ceu_1133
Definition: NPSMEFTd6.h:3609
double CuW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3568
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3576
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3504
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3509
double eZH_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3739
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3491
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3444
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3525
double eWH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3726
double CLL_2112
Definition: NPSMEFTd6.h:3592
double Ceu_3311
Definition: NPSMEFTd6.h:3609
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3466
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3520
double eZH_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3740
double CLQ3_1221
Definition: NPSMEFTd6.h:3600
double eVBF_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3693
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3651
double eZH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3745
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3541
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3648
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3513
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3457
double CLL_3113
Definition: NPSMEFTd6.h:3593
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3449
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3460
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3496
double CLd_1132
Definition: NPSMEFTd6.h:3627
double CLQ1_1331
Definition: NPSMEFTd6.h:3596
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of StandardModel.
double eZH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3741
double dKappaga
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:3797
double CQe_3222
Definition: NPSMEFTd6.h:3632
double CLu_3311
Definition: NPSMEFTd6.h:3621
double CLd_1122
Definition: NPSMEFTd6.h:3624
double CLe_1122
Definition: NPSMEFTd6.h:3617
double CLu_2233
Definition: NPSMEFTd6.h:3622
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients...
Definition: NPSMEFTd6.h:3906
double CLQ3_1133
Definition: NPSMEFTd6.h:3601
double CLedQ_11
Definition: NPSMEFTd6.h:3633
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3548
double CQe_3233
Definition: NPSMEFTd6.h:3632
double Ceu_2211
Definition: NPSMEFTd6.h:3608
double eWH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3733
double ettH_1314_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3788
double CLQ3_3113
Definition: NPSMEFTd6.h:3601
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3472
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3476
double eVBF_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3704
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3467
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3430
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3516
double eZH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3744
double CuB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3581
double CQe_2333
Definition: NPSMEFTd6.h:3631
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3551
double ettH_78_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3784
double CLQ3_1331
Definition: NPSMEFTd6.h:3601
double CuG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3562
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3531
double CQe_1122
Definition: NPSMEFTd6.h:3629
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3445
double Ceu_1111
Definition: NPSMEFTd6.h:3607
double eHggint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3652
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3523
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3486
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3446
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3495
double Ced_3332
Definition: NPSMEFTd6.h:3615
double CuB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3583
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3450
double ettH_78_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3783
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3572
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3459
double CLe_2211
Definition: NPSMEFTd6.h:3617
double eWH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3732
double eVBF_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3711
double eWH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3730
double CpLedQ_11
Definition: NPSMEFTd6.h:3633
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3434
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3470
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3546
bool FlagPartialQFU
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd fa...
Definition: NPSMEFTd6.h:3905
double Ced_2223
Definition: NPSMEFTd6.h:3614
double CLQ1_3113
Definition: NPSMEFTd6.h:3596
double CLu_2211
Definition: NPSMEFTd6.h:3620
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3582
double CuG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3565
double CLQ3_1132
Definition: NPSMEFTd6.h:3603
double ettH_2_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3779
double CLL_1122
Definition: NPSMEFTd6.h:3592
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3502
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3507
double CLd_2211
Definition: NPSMEFTd6.h:3624
double CQe_3211
Definition: NPSMEFTd6.h:3632
double eHccint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:3666
double CLQ1_2232
Definition: NPSMEFTd6.h:3598
double CLQ1_1122
Definition: NPSMEFTd6.h:3595
double eHgagapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3661
double CuW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3569
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3479
double CLd_3323
Definition: NPSMEFTd6.h:3626
double ettH_78_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3782
double eZH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3761
double eVBF_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3692
double eZH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3754
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3524
double eVBF_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3702
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:3794
double CuG_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3559
double CLd_3332
Definition: NPSMEFTd6.h:3627
double CLQ1_2223
Definition: NPSMEFTd6.h:3597
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3527
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3448
double ettH_1314_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:3789
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3498
double eWH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3713
double CLQ3_3311
Definition: NPSMEFTd6.h:3601
double CuW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3575
double eZHint
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3644
double eZH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3771
double eZH_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3769
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3505
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3534
double eZH_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3772
double eVBF_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3699
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3483
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3588
double eWHint
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3642
double eWH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3729
double CLd_3311
Definition: NPSMEFTd6.h:3625
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3517
double CLQ3_2211
Definition: NPSMEFTd6.h:3600
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3478
double eVBF_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3688
double eZH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3750
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:3646
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3578
double eWH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3717
double Cee_2211
Definition: NPSMEFTd6.h:3605
double CLQ1_1132
Definition: NPSMEFTd6.h:3598
double eVBF_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3677
double CuG_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3556
double eVBF_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3682
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3573
double CLQ3_3332
Definition: NPSMEFTd6.h:3603
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3500
double CQe_1111
Definition: NPSMEFTd6.h:3628
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3561
double Ced_2211
Definition: NPSMEFTd6.h:3612
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3503
double eZH_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3765
double CuW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3574
double ettH_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:3786
double CLQ1_1221
Definition: NPSMEFTd6.h:3595
double Ced_3311
Definition: NPSMEFTd6.h:3613
double CLd_2232
Definition: NPSMEFTd6.h:3627
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3458
double eHccpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3667
double CLu_1122
Definition: NPSMEFTd6.h:3620
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3499
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3440
double eWH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3715
double ettHint
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3638
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3539
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3439
double eZH_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3752
double eVBF_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3697
double eVBF_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3678
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:3793
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3484
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3533
double eWH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:3727
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3497
double CLL_3311
Definition: NPSMEFTd6.h:3593
double eHmumupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:3663
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3560
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3490
double eZH_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3751
double eVBF_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3679
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:3634
double CuG_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3557
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3465
double CLu_1111
Definition: NPSMEFTd6.h:3619
double eZH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3755
double CuB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3580
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3526
double eVBF_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3680
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3537
double Cee_1122
Definition: NPSMEFTd6.h:3605
double CHWHB_gaga
The combination of dimension-6 operator coefficients entering in : .
Definition: NPSMEFTd6.h:3436
double eZHpar
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3645
double eWH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3735
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:3471
double eggFint
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy...
Definition: NPSMEFTd6.h:3636
double CQe_3311
Definition: NPSMEFTd6.h:3630
double eZH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3770
double eWH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:3719
double eVBF_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3705
double eZH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3767
double eWH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:3731
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3487
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3475
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3451
double Ced_1122
Definition: NPSMEFTd6.h:3612
double eVBF_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3690
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3530
double eVBF_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3675
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3564
double Cee_1111
Definition: NPSMEFTd6.h:3604
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3454
double eZH_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3746
double CLe_1133
Definition: NPSMEFTd6.h:3618
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3455
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3545
double CQe_1133
Definition: NPSMEFTd6.h:3630
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:3488
double CLQ1_3332
Definition: NPSMEFTd6.h:3598
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3532
double eZH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:3757
double CQe_2311
Definition: NPSMEFTd6.h:3631
double eVBF_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3710
double eVBF_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:3708
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:3584

◆ xseeWW()

double NPSMEFTd6::xseeWW ( const double  sqrt_s) const
virtual

Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).

Returns
\(\sigma(e^+ e^- \to W^+ W^- \to jj \ell \nu) \)

Reimplemented from NPbase.

Definition at line 12577 of file NPSMEFTd6.cpp.

12578 {
12579  return dxseeWWdcosBin(sqrt_s, -1.0, 1.0);
12580 }
virtual double dxseeWWdcosBin(const double sqrt_s, const double cos1, const double cos2) const
The integral of differential distribution for , with in a given bin of the polar angle...

Member Data Documentation

◆ aleMz

double NPSMEFTd6::aleMz
protected

The em constant at Mz.

Definition at line 3802 of file NPSMEFTd6.h.

◆ BrHexo

double NPSMEFTd6::BrHexo
protected

The branching ratio of exotic (not invisible) Higgs decays.

Definition at line 3794 of file NPSMEFTd6.h.

◆ BrHinv

double NPSMEFTd6::BrHinv
protected

The branching ratio of invisible Higgs decays.

Definition at line 3793 of file NPSMEFTd6.h.

◆ C2B

double NPSMEFTd6::C2B
protected

The dimension-6 operator coefficient \(C_{2W}\).

Definition at line 3431 of file NPSMEFTd6.h.

◆ C2W

double NPSMEFTd6::C2W
protected

The dimension-6 operator coefficient \(C_{2B}\).

Definition at line 3432 of file NPSMEFTd6.h.

◆ CdH_11i

double NPSMEFTd6::CdH_11i
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).

Definition at line 3549 of file NPSMEFTd6.h.

◆ CdH_11r

double NPSMEFTd6::CdH_11r
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).

Definition at line 3543 of file NPSMEFTd6.h.

◆ CdH_12i

double NPSMEFTd6::CdH_12i
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).

Definition at line 3550 of file NPSMEFTd6.h.

◆ CdH_12r

double NPSMEFTd6::CdH_12r
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).

Definition at line 3544 of file NPSMEFTd6.h.

◆ CdH_13i

double NPSMEFTd6::CdH_13i
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).

Definition at line 3551 of file NPSMEFTd6.h.

◆ CdH_13r

double NPSMEFTd6::CdH_13r
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).

Definition at line 3545 of file NPSMEFTd6.h.

◆ CdH_22i

double NPSMEFTd6::CdH_22i
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).

Definition at line 3552 of file NPSMEFTd6.h.

◆ CdH_22r

double NPSMEFTd6::CdH_22r
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).

Definition at line 3546 of file NPSMEFTd6.h.

◆ CdH_23i

double NPSMEFTd6::CdH_23i
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).

Definition at line 3553 of file NPSMEFTd6.h.

◆ CdH_23r

double NPSMEFTd6::CdH_23r
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).

Definition at line 3547 of file NPSMEFTd6.h.

◆ CdH_33i

double NPSMEFTd6::CdH_33i
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).

Definition at line 3554 of file NPSMEFTd6.h.

◆ CdH_33r

double NPSMEFTd6::CdH_33r
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).

Definition at line 3548 of file NPSMEFTd6.h.

◆ CDHB

double NPSMEFTd6::CDHB
protected

The dimension-6 operator coefficient \(C_{DHB}\).

Definition at line 3438 of file NPSMEFTd6.h.

◆ CDHW

double NPSMEFTd6::CDHW
protected

The dimension-6 operator coefficient \(C_{DHW}\).

Definition at line 3439 of file NPSMEFTd6.h.

◆ Ced_1111

double NPSMEFTd6::Ced_1111
protected

Definition at line 3611 of file NPSMEFTd6.h.

◆ Ced_1122

double NPSMEFTd6::Ced_1122
protected

Definition at line 3612 of file NPSMEFTd6.h.

◆ Ced_1123

double NPSMEFTd6::Ced_1123
protected

Definition at line 3614 of file NPSMEFTd6.h.

◆ Ced_1132

double NPSMEFTd6::Ced_1132
protected

Definition at line 3615 of file NPSMEFTd6.h.

◆ Ced_1133

double NPSMEFTd6::Ced_1133
protected

Definition at line 3613 of file NPSMEFTd6.h.

◆ Ced_2211

double NPSMEFTd6::Ced_2211
protected

Definition at line 3612 of file NPSMEFTd6.h.

◆ Ced_2223

double NPSMEFTd6::Ced_2223
protected

Definition at line 3614 of file NPSMEFTd6.h.

◆ Ced_2232

double NPSMEFTd6::Ced_2232
protected

Definition at line 3615 of file NPSMEFTd6.h.

◆ Ced_3311

double NPSMEFTd6::Ced_3311
protected

Definition at line 3613 of file NPSMEFTd6.h.

◆ Ced_3323

double NPSMEFTd6::Ced_3323
protected

Definition at line 3614 of file NPSMEFTd6.h.

◆ Ced_3332

double NPSMEFTd6::Ced_3332
protected

Definition at line 3615 of file NPSMEFTd6.h.

◆ Cee_1111

double NPSMEFTd6::Cee_1111
protected

Definition at line 3604 of file NPSMEFTd6.h.

◆ Cee_1122

double NPSMEFTd6::Cee_1122
protected

Definition at line 3605 of file NPSMEFTd6.h.

◆ Cee_1133

double NPSMEFTd6::Cee_1133
protected

Definition at line 3606 of file NPSMEFTd6.h.

◆ Cee_2211

double NPSMEFTd6::Cee_2211
protected

Definition at line 3605 of file NPSMEFTd6.h.

◆ Cee_3311

double NPSMEFTd6::Cee_3311
protected

Definition at line 3606 of file NPSMEFTd6.h.

◆ CeH_11i

double NPSMEFTd6::CeH_11i
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).

Definition at line 3525 of file NPSMEFTd6.h.

◆ CeH_11r

double NPSMEFTd6::CeH_11r
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).

Definition at line 3519 of file NPSMEFTd6.h.

◆ CeH_12i

double NPSMEFTd6::CeH_12i
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).

Definition at line 3526 of file NPSMEFTd6.h.

◆ CeH_12r

double NPSMEFTd6::CeH_12r
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).

Definition at line 3520 of file NPSMEFTd6.h.

◆ CeH_13i

double NPSMEFTd6::CeH_13i
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).

Definition at line 3527 of file NPSMEFTd6.h.

◆ CeH_13r

double NPSMEFTd6::CeH_13r
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).

Definition at line 3521 of file NPSMEFTd6.h.

◆ CeH_22i

double NPSMEFTd6::CeH_22i
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).

Definition at line 3528 of file NPSMEFTd6.h.

◆ CeH_22r

double NPSMEFTd6::CeH_22r
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).

Definition at line 3522 of file NPSMEFTd6.h.

◆ CeH_23i

double NPSMEFTd6::CeH_23i
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).

Definition at line 3529 of file NPSMEFTd6.h.

◆ CeH_23r

double NPSMEFTd6::CeH_23r
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).

Definition at line 3523 of file NPSMEFTd6.h.

◆ CeH_33i

double NPSMEFTd6::CeH_33i
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).

Definition at line 3530 of file NPSMEFTd6.h.

◆ CeH_33r

double NPSMEFTd6::CeH_33r
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).

Definition at line 3524 of file NPSMEFTd6.h.

◆ Ceu_1111

double NPSMEFTd6::Ceu_1111
protected

Definition at line 3607 of file NPSMEFTd6.h.

◆ Ceu_1122

double NPSMEFTd6::Ceu_1122
protected

Definition at line 3608 of file NPSMEFTd6.h.

◆ Ceu_1133

double NPSMEFTd6::Ceu_1133
protected

Definition at line 3609 of file NPSMEFTd6.h.

◆ Ceu_2211

double NPSMEFTd6::Ceu_2211
protected

Definition at line 3608 of file NPSMEFTd6.h.

◆ Ceu_2233

double NPSMEFTd6::Ceu_2233
protected

Definition at line 3610 of file NPSMEFTd6.h.

◆ Ceu_3311

double NPSMEFTd6::Ceu_3311
protected

Definition at line 3609 of file NPSMEFTd6.h.

◆ CG

double NPSMEFTd6::CG
protected

The dimension-6 operator coefficient \(C_{G}\).

Definition at line 3429 of file NPSMEFTd6.h.

◆ CH

double NPSMEFTd6::CH
protected

The dimension-6 operator coefficient \(C_{H}\).

Definition at line 3443 of file NPSMEFTd6.h.

◆ CHB

double NPSMEFTd6::CHB
protected

The dimension-6 operator coefficient \(C_{HB}\).

Definition at line 3435 of file NPSMEFTd6.h.

◆ CHbox

double NPSMEFTd6::CHbox
protected

The dimension-6 operator coefficient \(C_{H\Box}\).

Definition at line 3442 of file NPSMEFTd6.h.

◆ CHD

double NPSMEFTd6::CHD
protected

The dimension-6 operator coefficient \(C_{HD}\).

Definition at line 3441 of file NPSMEFTd6.h.

◆ CHd_11

double NPSMEFTd6::CHd_11
protected

The dimension-6 operator coefficient \((C_{Hd})_{11}\).

Definition at line 3498 of file NPSMEFTd6.h.

◆ CHd_12i

double NPSMEFTd6::CHd_12i
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).

Definition at line 3504 of file NPSMEFTd6.h.

◆ CHd_12r

double NPSMEFTd6::CHd_12r
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).

Definition at line 3499 of file NPSMEFTd6.h.

◆ CHd_13i

double NPSMEFTd6::CHd_13i
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).

Definition at line 3505 of file NPSMEFTd6.h.

◆ CHd_13r

double NPSMEFTd6::CHd_13r
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).

Definition at line 3500 of file NPSMEFTd6.h.

◆ CHd_22

double NPSMEFTd6::CHd_22
protected

The dimension-6 operator coefficient \((C_{Hd})_{22}\).

Definition at line 3501 of file NPSMEFTd6.h.

◆ CHd_23i

double NPSMEFTd6::CHd_23i
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).

Definition at line 3506 of file NPSMEFTd6.h.

◆ CHd_23r

double NPSMEFTd6::CHd_23r
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).

Definition at line 3502 of file NPSMEFTd6.h.

◆ CHd_33

double NPSMEFTd6::CHd_33
protected

The dimension-6 operator coefficient \((C_{Hd})_{33}\).

Definition at line 3503 of file NPSMEFTd6.h.

◆ CHe_11

double NPSMEFTd6::CHe_11
protected

The dimension-6 operator coefficient \((C_{He})_{11}\).

Definition at line 3462 of file NPSMEFTd6.h.

◆ CHe_12i

double NPSMEFTd6::CHe_12i
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).

Definition at line 3468 of file NPSMEFTd6.h.

◆ CHe_12r

double NPSMEFTd6::CHe_12r
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).

Definition at line 3463 of file NPSMEFTd6.h.

◆ CHe_13i

double NPSMEFTd6::CHe_13i
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).

Definition at line 3469 of file NPSMEFTd6.h.

◆ CHe_13r

double NPSMEFTd6::CHe_13r
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).

Definition at line 3464 of file NPSMEFTd6.h.

◆ CHe_22

double NPSMEFTd6::CHe_22
protected

The dimension-6 operator coefficient \((C_{He})_{22}\).

Definition at line 3465 of file NPSMEFTd6.h.

◆ CHe_23i

double NPSMEFTd6::CHe_23i
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).

Definition at line 3470 of file NPSMEFTd6.h.

◆ CHe_23r

double NPSMEFTd6::CHe_23r
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).

Definition at line 3466 of file NPSMEFTd6.h.

◆ CHe_33

double NPSMEFTd6::CHe_33
protected

The dimension-6 operator coefficient \((C_{He})_{33}\).

Definition at line 3467 of file NPSMEFTd6.h.

◆ CHG

double NPSMEFTd6::CHG
protected

The dimension-6 operator coefficient \(C_{HG}\).

Definition at line 3433 of file NPSMEFTd6.h.

◆ CHL1_11

double NPSMEFTd6::CHL1_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).

Definition at line 3444 of file NPSMEFTd6.h.

◆ CHL1_12i

double NPSMEFTd6::CHL1_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).

Definition at line 3450 of file NPSMEFTd6.h.

◆ CHL1_12r

double NPSMEFTd6::CHL1_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).

Definition at line 3445 of file NPSMEFTd6.h.

◆ CHL1_13i

double NPSMEFTd6::CHL1_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).

Definition at line 3451 of file NPSMEFTd6.h.

◆ CHL1_13r

double NPSMEFTd6::CHL1_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).

Definition at line 3446 of file NPSMEFTd6.h.

◆ CHL1_22

double NPSMEFTd6::CHL1_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).

Definition at line 3447 of file NPSMEFTd6.h.

◆ CHL1_23i

double NPSMEFTd6::CHL1_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).

Definition at line 3452 of file NPSMEFTd6.h.

◆ CHL1_23r

double NPSMEFTd6::CHL1_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).

Definition at line 3448 of file NPSMEFTd6.h.

◆ CHL1_33

double NPSMEFTd6::CHL1_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).

Definition at line 3449 of file NPSMEFTd6.h.

◆ CHL3_11

double NPSMEFTd6::CHL3_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).

Definition at line 3453 of file NPSMEFTd6.h.

◆ CHL3_12i

double NPSMEFTd6::CHL3_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 3459 of file NPSMEFTd6.h.

◆ CHL3_12r

double NPSMEFTd6::CHL3_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 3454 of file NPSMEFTd6.h.

◆ CHL3_13i

double NPSMEFTd6::CHL3_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 3460 of file NPSMEFTd6.h.

◆ CHL3_13r

double NPSMEFTd6::CHL3_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 3455 of file NPSMEFTd6.h.

◆ CHL3_22

double NPSMEFTd6::CHL3_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).

Definition at line 3456 of file NPSMEFTd6.h.

◆ CHL3_23i

double NPSMEFTd6::CHL3_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 3461 of file NPSMEFTd6.h.

◆ CHL3_23r

double NPSMEFTd6::CHL3_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 3457 of file NPSMEFTd6.h.

◆ CHL3_33

double NPSMEFTd6::CHL3_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).

Definition at line 3458 of file NPSMEFTd6.h.

◆ CHQ1_11

double NPSMEFTd6::CHQ1_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).

Definition at line 3471 of file NPSMEFTd6.h.

◆ CHQ1_12i

double NPSMEFTd6::CHQ1_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).

Definition at line 3477 of file NPSMEFTd6.h.

◆ CHQ1_12r

double NPSMEFTd6::CHQ1_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).

Definition at line 3472 of file NPSMEFTd6.h.

◆ CHQ1_13i

double NPSMEFTd6::CHQ1_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).

Definition at line 3478 of file NPSMEFTd6.h.

◆ CHQ1_13r

double NPSMEFTd6::CHQ1_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).

Definition at line 3473 of file NPSMEFTd6.h.

◆ CHQ1_22

double NPSMEFTd6::CHQ1_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).

Definition at line 3474 of file NPSMEFTd6.h.

◆ CHQ1_23i

double NPSMEFTd6::CHQ1_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).

Definition at line 3479 of file NPSMEFTd6.h.

◆ CHQ1_23r

double NPSMEFTd6::CHQ1_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).

Definition at line 3475 of file NPSMEFTd6.h.

◆ CHQ1_33

double NPSMEFTd6::CHQ1_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).

Definition at line 3476 of file NPSMEFTd6.h.

◆ CHQ3_11

double NPSMEFTd6::CHQ3_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).

Definition at line 3480 of file NPSMEFTd6.h.

◆ CHQ3_12i

double NPSMEFTd6::CHQ3_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).

Definition at line 3486 of file NPSMEFTd6.h.

◆ CHQ3_12r

double NPSMEFTd6::CHQ3_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).

Definition at line 3481 of file NPSMEFTd6.h.

◆ CHQ3_13i

double NPSMEFTd6::CHQ3_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).

Definition at line 3487 of file NPSMEFTd6.h.

◆ CHQ3_13r

double NPSMEFTd6::CHQ3_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).

Definition at line 3482 of file NPSMEFTd6.h.

◆ CHQ3_22

double NPSMEFTd6::CHQ3_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).

Definition at line 3483 of file NPSMEFTd6.h.

◆ CHQ3_23i

double NPSMEFTd6::CHQ3_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).

Definition at line 3488 of file NPSMEFTd6.h.

◆ CHQ3_23r

double NPSMEFTd6::CHQ3_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).

Definition at line 3484 of file NPSMEFTd6.h.

◆ CHQ3_33

double NPSMEFTd6::CHQ3_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).

Definition at line 3485 of file NPSMEFTd6.h.

◆ cHSM

double NPSMEFTd6::cHSM
protected

Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.

Definition at line 3830 of file NPSMEFTd6.h.

◆ CHu_11

double NPSMEFTd6::CHu_11
protected

The dimension-6 operator coefficient \((C_{Hu})_{11}\).

Definition at line 3489 of file NPSMEFTd6.h.

◆ CHu_12i

double NPSMEFTd6::CHu_12i
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).

Definition at line 3495 of file NPSMEFTd6.h.

◆ CHu_12r

double NPSMEFTd6::CHu_12r
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).

Definition at line 3490 of file NPSMEFTd6.h.

◆ CHu_13i

double NPSMEFTd6::CHu_13i
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).

Definition at line 3496 of file NPSMEFTd6.h.

◆ CHu_13r

double NPSMEFTd6::CHu_13r
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).

Definition at line 3491 of file NPSMEFTd6.h.

◆ CHu_22

double NPSMEFTd6::CHu_22
protected

The dimension-6 operator coefficient \((C_{Hu})_{22}\).

Definition at line 3492 of file NPSMEFTd6.h.

◆ CHu_23i

double NPSMEFTd6::CHu_23i
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).

Definition at line 3497 of file NPSMEFTd6.h.

◆ CHu_23r

double NPSMEFTd6::CHu_23r
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).

Definition at line 3493 of file NPSMEFTd6.h.

◆ CHu_33

double NPSMEFTd6::CHu_33
protected

The dimension-6 operator coefficient \((C_{Hu})_{33}\).

Definition at line 3494 of file NPSMEFTd6.h.

◆ CHud_11i

double NPSMEFTd6::CHud_11i
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).

Definition at line 3513 of file NPSMEFTd6.h.

◆ CHud_11r

double NPSMEFTd6::CHud_11r
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).

Definition at line 3507 of file NPSMEFTd6.h.

◆ CHud_12i

double NPSMEFTd6::CHud_12i
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).

Definition at line 3514 of file NPSMEFTd6.h.

◆ CHud_12r

double NPSMEFTd6::CHud_12r
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).

Definition at line 3508 of file NPSMEFTd6.h.

◆ CHud_13i

double NPSMEFTd6::CHud_13i
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).

Definition at line 3515 of file NPSMEFTd6.h.

◆ CHud_13r

double NPSMEFTd6::CHud_13r
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).

Definition at line 3509 of file NPSMEFTd6.h.

◆ CHud_22i

double NPSMEFTd6::CHud_22i
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).

Definition at line 3516 of file NPSMEFTd6.h.

◆ CHud_22r

double NPSMEFTd6::CHud_22r
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).

Definition at line 3510 of file NPSMEFTd6.h.

◆ CHud_23i

double NPSMEFTd6::CHud_23i
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).

Definition at line 3517 of file NPSMEFTd6.h.

◆ CHud_23r

double NPSMEFTd6::CHud_23r
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).

Definition at line 3511 of file NPSMEFTd6.h.

◆ CHud_33i

double NPSMEFTd6::CHud_33i
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).

Definition at line 3518 of file NPSMEFTd6.h.

◆ CHud_33r

double NPSMEFTd6::CHud_33r
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).

Definition at line 3512 of file NPSMEFTd6.h.

◆ CHW

double NPSMEFTd6::CHW
protected

The dimension-6 operator coefficient \(C_{HW}\).

Definition at line 3434 of file NPSMEFTd6.h.

◆ CHWB

double NPSMEFTd6::CHWB
protected

The dimension-6 operator coefficient \(C_{HWB}\).

Definition at line 3440 of file NPSMEFTd6.h.

◆ CHWHB_gaga

double NPSMEFTd6::CHWHB_gaga
protected

The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).

Definition at line 3436 of file NPSMEFTd6.h.

◆ CHWHB_gagaorth

double NPSMEFTd6::CHWHB_gagaorth
protected

The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).

Definition at line 3437 of file NPSMEFTd6.h.

◆ CLd_1111

double NPSMEFTd6::CLd_1111
protected

Definition at line 3623 of file NPSMEFTd6.h.

◆ CLd_1122

double NPSMEFTd6::CLd_1122
protected

Definition at line 3624 of file NPSMEFTd6.h.

◆ CLd_1123

double NPSMEFTd6::CLd_1123
protected

Definition at line 3626 of file NPSMEFTd6.h.

◆ CLd_1132

double NPSMEFTd6::CLd_1132
protected

Definition at line 3627 of file NPSMEFTd6.h.

◆ CLd_1133

double NPSMEFTd6::CLd_1133
protected

Definition at line 3625 of file NPSMEFTd6.h.

◆ CLd_2211

double NPSMEFTd6::CLd_2211
protected

Definition at line 3624 of file NPSMEFTd6.h.

◆ CLd_2223

double NPSMEFTd6::CLd_2223
protected

Definition at line 3626 of file NPSMEFTd6.h.

◆ CLd_2232

double NPSMEFTd6::CLd_2232
protected

Definition at line 3627 of file NPSMEFTd6.h.

◆ CLd_3311

double NPSMEFTd6::CLd_3311
protected

Definition at line 3625 of file NPSMEFTd6.h.

◆ CLd_3323

double NPSMEFTd6::CLd_3323
protected

Definition at line 3626 of file NPSMEFTd6.h.

◆ CLd_3332

double NPSMEFTd6::CLd_3332
protected

Definition at line 3627 of file NPSMEFTd6.h.

◆ CLe_1111

double NPSMEFTd6::CLe_1111
protected

Definition at line 3616 of file NPSMEFTd6.h.

◆ CLe_1122

double NPSMEFTd6::CLe_1122
protected

Definition at line 3617 of file NPSMEFTd6.h.

◆ CLe_1133

double NPSMEFTd6::CLe_1133
protected

Definition at line 3618 of file NPSMEFTd6.h.

◆ CLe_2211

double NPSMEFTd6::CLe_2211
protected

Definition at line 3617 of file NPSMEFTd6.h.

◆ CLe_3311

double NPSMEFTd6::CLe_3311
protected

Definition at line 3618 of file NPSMEFTd6.h.

◆ CLedQ_11

double NPSMEFTd6::CLedQ_11
protected

Definition at line 3633 of file NPSMEFTd6.h.

◆ CLedQ_22

double NPSMEFTd6::CLedQ_22
protected

Definition at line 3633 of file NPSMEFTd6.h.

◆ cLH3d62

double NPSMEFTd6::cLH3d62
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).

Definition at line 3834 of file NPSMEFTd6.h.

◆ cLHd6

double NPSMEFTd6::cLHd6
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.

Definition at line 3832 of file NPSMEFTd6.h.

◆ CLL_1111

double NPSMEFTd6::CLL_1111
protected

Definition at line 3591 of file NPSMEFTd6.h.

◆ CLL_1122

double NPSMEFTd6::CLL_1122
protected

Definition at line 3592 of file NPSMEFTd6.h.

◆ CLL_1133

double NPSMEFTd6::CLL_1133
protected

Definition at line 3593 of file NPSMEFTd6.h.

◆ CLL_1221

double NPSMEFTd6::CLL_1221
protected

Definition at line 3592 of file NPSMEFTd6.h.

◆ CLL_1331

double NPSMEFTd6::CLL_1331
protected

Definition at line 3593 of file NPSMEFTd6.h.

◆ CLL_2112

double NPSMEFTd6::CLL_2112
protected

Definition at line 3592 of file NPSMEFTd6.h.

◆ CLL_2211

double NPSMEFTd6::CLL_2211
protected

Definition at line 3592 of file NPSMEFTd6.h.

◆ CLL_3113

double NPSMEFTd6::CLL_3113
protected

Definition at line 3593 of file NPSMEFTd6.h.

◆ CLL_3311

double NPSMEFTd6::CLL_3311
protected

Definition at line 3593 of file NPSMEFTd6.h.

◆ CLQ1_1111

double NPSMEFTd6::CLQ1_1111
protected

Definition at line 3594 of file NPSMEFTd6.h.

◆ CLQ1_1122

double NPSMEFTd6::CLQ1_1122
protected

Definition at line 3595 of file NPSMEFTd6.h.

◆ CLQ1_1123

double NPSMEFTd6::CLQ1_1123
protected

Definition at line 3597 of file NPSMEFTd6.h.

◆ CLQ1_1132

double NPSMEFTd6::CLQ1_1132
protected

Definition at line 3598 of file NPSMEFTd6.h.

◆ CLQ1_1133

double NPSMEFTd6::CLQ1_1133
protected

Definition at line 3596 of file NPSMEFTd6.h.

◆ CLQ1_1221

double NPSMEFTd6::CLQ1_1221
protected

Definition at line 3595 of file NPSMEFTd6.h.

◆ CLQ1_1331

double NPSMEFTd6::CLQ1_1331
protected

Definition at line 3596 of file NPSMEFTd6.h.

◆ CLQ1_2112

double NPSMEFTd6::CLQ1_2112
protected

Definition at line 3595 of file NPSMEFTd6.h.

◆ CLQ1_2211

double NPSMEFTd6::CLQ1_2211
protected

Definition at line 3595 of file NPSMEFTd6.h.

◆ CLQ1_2223

double NPSMEFTd6::CLQ1_2223
protected

Definition at line 3597 of file NPSMEFTd6.h.

◆ CLQ1_2232

double NPSMEFTd6::CLQ1_2232
protected

Definition at line 3598 of file NPSMEFTd6.h.

◆ CLQ1_3113

double NPSMEFTd6::CLQ1_3113
protected

Definition at line 3596 of file NPSMEFTd6.h.

◆ CLQ1_3311

double NPSMEFTd6::CLQ1_3311
protected

Definition at line 3596 of file NPSMEFTd6.h.

◆ CLQ1_3323

double NPSMEFTd6::CLQ1_3323
protected

Definition at line 3597 of file NPSMEFTd6.h.

◆ CLQ1_3332

double NPSMEFTd6::CLQ1_3332
protected

Definition at line 3598 of file NPSMEFTd6.h.

◆ CLQ3_1111

double NPSMEFTd6::CLQ3_1111
protected

Definition at line 3599 of file NPSMEFTd6.h.

◆ CLQ3_1122

double NPSMEFTd6::CLQ3_1122
protected

Definition at line 3600 of file NPSMEFTd6.h.

◆ CLQ3_1123

double NPSMEFTd6::CLQ3_1123
protected

Definition at line 3602 of file NPSMEFTd6.h.

◆ CLQ3_1132

double NPSMEFTd6::CLQ3_1132
protected

Definition at line 3603 of file NPSMEFTd6.h.

◆ CLQ3_1133

double NPSMEFTd6::CLQ3_1133
protected

Definition at line 3601 of file NPSMEFTd6.h.

◆ CLQ3_1221

double NPSMEFTd6::CLQ3_1221
protected

Definition at line 3600 of file NPSMEFTd6.h.

◆ CLQ3_1331

double NPSMEFTd6::CLQ3_1331
protected

Definition at line 3601 of file NPSMEFTd6.h.

◆ CLQ3_2112

double NPSMEFTd6::CLQ3_2112
protected

Definition at line 3600 of file NPSMEFTd6.h.

◆ CLQ3_2211

double NPSMEFTd6::CLQ3_2211
protected

Definition at line 3600 of file NPSMEFTd6.h.

◆ CLQ3_2223

double NPSMEFTd6::CLQ3_2223
protected

Definition at line 3602 of file NPSMEFTd6.h.

◆ CLQ3_2232

double NPSMEFTd6::CLQ3_2232
protected

Definition at line 3603 of file NPSMEFTd6.h.

◆ CLQ3_3113

double NPSMEFTd6::CLQ3_3113
protected

Definition at line 3601 of file NPSMEFTd6.h.

◆ CLQ3_3311

double NPSMEFTd6::CLQ3_3311
protected

Definition at line 3601 of file NPSMEFTd6.h.

◆ CLQ3_3323

double NPSMEFTd6::CLQ3_3323
protected

Definition at line 3602 of file NPSMEFTd6.h.

◆ CLQ3_3332

double NPSMEFTd6::CLQ3_3332
protected

Definition at line 3603 of file NPSMEFTd6.h.

◆ CLu_1111

double NPSMEFTd6::CLu_1111
protected

Definition at line 3619 of file NPSMEFTd6.h.

◆ CLu_1122

double NPSMEFTd6::CLu_1122
protected

Definition at line 3620 of file NPSMEFTd6.h.

◆ CLu_1133

double NPSMEFTd6::CLu_1133
protected

Definition at line 3621 of file NPSMEFTd6.h.

◆ CLu_2211

double NPSMEFTd6::CLu_2211
protected

Definition at line 3620 of file NPSMEFTd6.h.

◆ CLu_2233

double NPSMEFTd6::CLu_2233
protected

Definition at line 3622 of file NPSMEFTd6.h.

◆ CLu_3311

double NPSMEFTd6::CLu_3311
protected

Definition at line 3621 of file NPSMEFTd6.h.

◆ CpLedQ_11

double NPSMEFTd6::CpLedQ_11
protected

Definition at line 3633 of file NPSMEFTd6.h.

◆ CpLedQ_22

double NPSMEFTd6::CpLedQ_22
protected

Definition at line 3633 of file NPSMEFTd6.h.

◆ CQe_1111

double NPSMEFTd6::CQe_1111
protected

Definition at line 3628 of file NPSMEFTd6.h.

◆ CQe_1122

double NPSMEFTd6::CQe_1122
protected

Definition at line 3629 of file NPSMEFTd6.h.

◆ CQe_1133

double NPSMEFTd6::CQe_1133
protected

Definition at line 3630 of file NPSMEFTd6.h.

◆ CQe_2211

double NPSMEFTd6::CQe_2211
protected

Definition at line 3629 of file NPSMEFTd6.h.

◆ CQe_2311

double NPSMEFTd6::CQe_2311
protected

Definition at line 3631 of file NPSMEFTd6.h.

◆ CQe_2322

double NPSMEFTd6::CQe_2322
protected

Definition at line 3631 of file NPSMEFTd6.h.

◆ CQe_2333

double NPSMEFTd6::CQe_2333
protected

Definition at line 3631 of file NPSMEFTd6.h.

◆ CQe_3211

double NPSMEFTd6::CQe_3211
protected

Definition at line 3632 of file NPSMEFTd6.h.

◆ CQe_3222

double NPSMEFTd6::CQe_3222
protected

Definition at line 3632 of file NPSMEFTd6.h.

◆ CQe_3233

double NPSMEFTd6::CQe_3233
protected

Definition at line 3632 of file NPSMEFTd6.h.

◆ CQe_3311

double NPSMEFTd6::CQe_3311
protected

Definition at line 3630 of file NPSMEFTd6.h.

◆ CuB_11i

double NPSMEFTd6::CuB_11i
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).

Definition at line 3585 of file NPSMEFTd6.h.

◆ CuB_11r

double NPSMEFTd6::CuB_11r
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).

Definition at line 3579 of file NPSMEFTd6.h.

◆ CuB_12i

double NPSMEFTd6::CuB_12i
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).

Definition at line 3586 of file NPSMEFTd6.h.

◆ CuB_12r

double NPSMEFTd6::CuB_12r
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).

Definition at line 3580 of file NPSMEFTd6.h.

◆ CuB_13i

double NPSMEFTd6::CuB_13i
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).

Definition at line 3587 of file NPSMEFTd6.h.

◆ CuB_13r

double NPSMEFTd6::CuB_13r
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).

Definition at line 3581 of file NPSMEFTd6.h.

◆ CuB_22i

double NPSMEFTd6::CuB_22i
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).

Definition at line 3588 of file NPSMEFTd6.h.

◆ CuB_22r

double NPSMEFTd6::CuB_22r
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).

Definition at line 3582 of file NPSMEFTd6.h.

◆ CuB_23i

double NPSMEFTd6::CuB_23i
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).

Definition at line 3589 of file NPSMEFTd6.h.

◆ CuB_23r

double NPSMEFTd6::CuB_23r
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).

Definition at line 3583 of file NPSMEFTd6.h.

◆ CuB_33i

double NPSMEFTd6::CuB_33i
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).

Definition at line 3590 of file NPSMEFTd6.h.

◆ CuB_33r

double NPSMEFTd6::CuB_33r
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).

Definition at line 3584 of file NPSMEFTd6.h.

◆ CuG_11i

double NPSMEFTd6::CuG_11i
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).

Definition at line 3561 of file NPSMEFTd6.h.

◆ CuG_11r

double NPSMEFTd6::CuG_11r
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).

Definition at line 3555 of file NPSMEFTd6.h.

◆ CuG_12i

double NPSMEFTd6::CuG_12i
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).

Definition at line 3562 of file NPSMEFTd6.h.

◆ CuG_12r

double NPSMEFTd6::CuG_12r
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).

Definition at line 3556 of file NPSMEFTd6.h.

◆ CuG_13i

double NPSMEFTd6::CuG_13i
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).

Definition at line 3563 of file NPSMEFTd6.h.

◆ CuG_13r

double NPSMEFTd6::CuG_13r
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).

Definition at line 3557 of file NPSMEFTd6.h.

◆ CuG_22i

double NPSMEFTd6::CuG_22i
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).

Definition at line 3564 of file NPSMEFTd6.h.

◆ CuG_22r

double NPSMEFTd6::CuG_22r
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).

Definition at line 3558 of file NPSMEFTd6.h.

◆ CuG_23i

double NPSMEFTd6::CuG_23i
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).

Definition at line 3565 of file NPSMEFTd6.h.

◆ CuG_23r

double NPSMEFTd6::CuG_23r
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).

Definition at line 3559 of file NPSMEFTd6.h.

◆ CuG_33i

double NPSMEFTd6::CuG_33i
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).

Definition at line 3566 of file NPSMEFTd6.h.

◆ CuG_33r

double NPSMEFTd6::CuG_33r
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).

Definition at line 3560 of file NPSMEFTd6.h.

◆ CuH_11i

double NPSMEFTd6::CuH_11i
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).

Definition at line 3537 of file NPSMEFTd6.h.

◆ CuH_11r

double NPSMEFTd6::CuH_11r
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).

Definition at line 3531 of file NPSMEFTd6.h.

◆ CuH_12i

double NPSMEFTd6::CuH_12i
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).

Definition at line 3538 of file NPSMEFTd6.h.

◆ CuH_12r

double NPSMEFTd6::CuH_12r
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).

Definition at line 3532 of file NPSMEFTd6.h.

◆ CuH_13i

double NPSMEFTd6::CuH_13i
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).

Definition at line 3539 of file NPSMEFTd6.h.

◆ CuH_13r

double NPSMEFTd6::CuH_13r
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).

Definition at line 3533 of file NPSMEFTd6.h.

◆ CuH_22i

double NPSMEFTd6::CuH_22i
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).

Definition at line 3540 of file NPSMEFTd6.h.

◆ CuH_22r

double NPSMEFTd6::CuH_22r
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).

Definition at line 3534 of file NPSMEFTd6.h.

◆ CuH_23i

double NPSMEFTd6::CuH_23i
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).

Definition at line 3541 of file NPSMEFTd6.h.

◆ CuH_23r

double NPSMEFTd6::CuH_23r
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).

Definition at line 3535 of file NPSMEFTd6.h.

◆ CuH_33i

double NPSMEFTd6::CuH_33i
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).

Definition at line 3542 of file NPSMEFTd6.h.

◆ CuH_33r

double NPSMEFTd6::CuH_33r
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).

Definition at line 3536 of file NPSMEFTd6.h.

◆ CuW_11i

double NPSMEFTd6::CuW_11i
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).

Definition at line 3573 of file NPSMEFTd6.h.

◆ CuW_11r

double NPSMEFTd6::CuW_11r
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).

Definition at line 3567 of file NPSMEFTd6.h.

◆ CuW_12i

double NPSMEFTd6::CuW_12i
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).

Definition at line 3574 of file NPSMEFTd6.h.

◆ CuW_12r

double NPSMEFTd6::CuW_12r
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).

Definition at line 3568 of file NPSMEFTd6.h.

◆ CuW_13i

double NPSMEFTd6::CuW_13i
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).

Definition at line 3575 of file NPSMEFTd6.h.

◆ CuW_13r

double NPSMEFTd6::CuW_13r
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).

Definition at line 3569 of file NPSMEFTd6.h.

◆ CuW_22i

double NPSMEFTd6::CuW_22i
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).

Definition at line 3576 of file NPSMEFTd6.h.

◆ CuW_22r

double NPSMEFTd6::CuW_22r
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).

Definition at line 3570 of file NPSMEFTd6.h.

◆ CuW_23i

double NPSMEFTd6::CuW_23i
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).

Definition at line 3577 of file NPSMEFTd6.h.

◆ CuW_23r

double NPSMEFTd6::CuW_23r
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).

Definition at line 3571 of file NPSMEFTd6.h.

◆ CuW_33i

double NPSMEFTd6::CuW_33i
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).

Definition at line 3578 of file NPSMEFTd6.h.

◆ CuW_33r

double NPSMEFTd6::CuW_33r
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).

Definition at line 3572 of file NPSMEFTd6.h.

◆ CW

double NPSMEFTd6::CW
protected

The dimension-6 operator coefficient \(C_{W}\).

Definition at line 3430 of file NPSMEFTd6.h.

◆ cW2_tree

double NPSMEFTd6::cW2_tree
protected

The square of the tree level values for the cosine of the weak angle.

Definition at line 3807 of file NPSMEFTd6.h.

◆ cW_tree

double NPSMEFTd6::cW_tree
protected

The tree level values for the cosine of the weak angle.

Definition at line 3805 of file NPSMEFTd6.h.

◆ delta_AA

double NPSMEFTd6::delta_AA
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 3822 of file NPSMEFTd6.h.

◆ delta_AZ

double NPSMEFTd6::delta_AZ
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 3823 of file NPSMEFTd6.h.

◆ delta_h

double NPSMEFTd6::delta_h
protected

Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.

Definition at line 3824 of file NPSMEFTd6.h.

◆ delta_ZZ

double NPSMEFTd6::delta_ZZ
protected

Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.

Definition at line 3821 of file NPSMEFTd6.h.

◆ dg1Z

double NPSMEFTd6::dg1Z
protected

Independent contribution to aTGC.

Definition at line 3796 of file NPSMEFTd6.h.

◆ dGammaHTotR1

double NPSMEFTd6::dGammaHTotR1
protected

Definition at line 3841 of file NPSMEFTd6.h.

◆ dGammaHTotR2

double NPSMEFTd6::dGammaHTotR2
protected

Definition at line 3841 of file NPSMEFTd6.h.

◆ dKappaga

double NPSMEFTd6::dKappaga
protected

Independent contribution to aTGC.

Definition at line 3797 of file NPSMEFTd6.h.

◆ dZH

double NPSMEFTd6::dZH
protected

Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.

Definition at line 3828 of file NPSMEFTd6.h.

◆ eeettHint

double NPSMEFTd6::eeettHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 3650 of file NPSMEFTd6.h.

◆ eeettHpar

double NPSMEFTd6::eeettHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 3651 of file NPSMEFTd6.h.

◆ eeeWBFint

double NPSMEFTd6::eeeWBFint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 3646 of file NPSMEFTd6.h.

◆ eeeWBFpar

double NPSMEFTd6::eeeWBFpar
protected

Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 3647 of file NPSMEFTd6.h.

◆ eeeZHint

double NPSMEFTd6::eeeZHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 3648 of file NPSMEFTd6.h.

◆ eeeZHpar

double NPSMEFTd6::eeeZHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 3649 of file NPSMEFTd6.h.

◆ eeMz

double NPSMEFTd6::eeMz
protected

The em coupling at Mz.

Definition at line 3803 of file NPSMEFTd6.h.

◆ eeMz2

double NPSMEFTd6::eeMz2
protected

The em coupling squared (at Mz).

Definition at line 3804 of file NPSMEFTd6.h.

◆ eggFint

double NPSMEFTd6::eggFint
protected

Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 3636 of file NPSMEFTd6.h.

◆ eggFpar

double NPSMEFTd6::eggFpar
protected

Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 3637 of file NPSMEFTd6.h.

◆ eHbbint

double NPSMEFTd6::eHbbint
protected

Intrinsic relative theoretical error in \(H \to b\bar{b}\).

Definition at line 3668 of file NPSMEFTd6.h.

◆ eHbbpar

double NPSMEFTd6::eHbbpar
protected

Parametric relative theoretical error in \(H \to b\bar{b}\).

Definition at line 3669 of file NPSMEFTd6.h.

◆ eHccint

double NPSMEFTd6::eHccint
protected

Intrinsic relative theoretical error in \(H \to c\bar{c}\).

Definition at line 3666 of file NPSMEFTd6.h.

◆ eHccpar

double NPSMEFTd6::eHccpar
protected

Parametric relative theoretical error in \(H \to c\bar{c}\).

Definition at line 3667 of file NPSMEFTd6.h.

◆ eHgagaint

double NPSMEFTd6::eHgagaint
protected

Intrinsic relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 3660 of file NPSMEFTd6.h.

◆ eHgagapar

double NPSMEFTd6::eHgagapar
protected

Parametric relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 3661 of file NPSMEFTd6.h.

◆ eHggint

double NPSMEFTd6::eHggint
protected

Intrinsic relative theoretical error in \(H \to g g\).

Definition at line 3652 of file NPSMEFTd6.h.

◆ eHggpar

double NPSMEFTd6::eHggpar
protected

Parametric relative theoretical error in \(H \to g g\).

Definition at line 3653 of file NPSMEFTd6.h.

◆ eHmumuint

double NPSMEFTd6::eHmumuint
protected

Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 3662 of file NPSMEFTd6.h.

◆ eHmumupar

double NPSMEFTd6::eHmumupar
protected

Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 3663 of file NPSMEFTd6.h.

◆ eHtautauint

double NPSMEFTd6::eHtautauint
protected

Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 3664 of file NPSMEFTd6.h.

◆ eHtautaupar

double NPSMEFTd6::eHtautaupar
protected

Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 3665 of file NPSMEFTd6.h.

◆ eHWWint

double NPSMEFTd6::eHWWint
protected

Intrinsic relative theoretical error in \(H \to W W\).

Definition at line 3654 of file NPSMEFTd6.h.

◆ eHWWpar

double NPSMEFTd6::eHWWpar
protected

Parametric relative theoretical error in \(H \to W W\).

Definition at line 3655 of file NPSMEFTd6.h.

◆ eHZgaint

double NPSMEFTd6::eHZgaint
protected

Intrinsic relative theoretical error in \(H \to Z \gamma\).

Definition at line 3658 of file NPSMEFTd6.h.

◆ eHZgapar

double NPSMEFTd6::eHZgapar
protected

Parametric relative theoretical error in \(H \to Z \gamma\).

Definition at line 3659 of file NPSMEFTd6.h.

◆ eHZZint

double NPSMEFTd6::eHZZint
protected

Intrinsic relative theoretical error in \(H \to Z Z\).

Definition at line 3656 of file NPSMEFTd6.h.

◆ eHZZpar

double NPSMEFTd6::eHZZpar
protected

Parametric relative theoretical error in \(H \to Z Z\).

Definition at line 3657 of file NPSMEFTd6.h.

◆ ettH_1314_DeltagHt

double NPSMEFTd6::ettH_1314_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 3789 of file NPSMEFTd6.h.

◆ ettH_1314_G

double NPSMEFTd6::ettH_1314_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 3787 of file NPSMEFTd6.h.

◆ ettH_1314_HG

double NPSMEFTd6::ettH_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 3786 of file NPSMEFTd6.h.

◆ ettH_1314_uG_33r

double NPSMEFTd6::ettH_1314_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 3788 of file NPSMEFTd6.h.

◆ ettH_2_DeltagHt

double NPSMEFTd6::ettH_2_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).

Definition at line 3779 of file NPSMEFTd6.h.

◆ ettH_2_G

double NPSMEFTd6::ettH_2_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 3777 of file NPSMEFTd6.h.

◆ ettH_2_HG

double NPSMEFTd6::ettH_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 3776 of file NPSMEFTd6.h.

◆ ettH_2_uG_33r

double NPSMEFTd6::ettH_2_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).

Definition at line 3778 of file NPSMEFTd6.h.

◆ ettH_78_DeltagHt

double NPSMEFTd6::ettH_78_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 3784 of file NPSMEFTd6.h.

◆ ettH_78_G

double NPSMEFTd6::ettH_78_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 3782 of file NPSMEFTd6.h.

◆ ettH_78_HG

double NPSMEFTd6::ettH_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 3781 of file NPSMEFTd6.h.

◆ ettH_78_uG_33r

double NPSMEFTd6::ettH_78_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 3783 of file NPSMEFTd6.h.

◆ ettHint

double NPSMEFTd6::ettHint
protected

Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 3638 of file NPSMEFTd6.h.

◆ ettHpar

double NPSMEFTd6::ettHpar
protected

Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 3639 of file NPSMEFTd6.h.

◆ eVBF_1314_DeltaGF

double NPSMEFTd6::eVBF_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3711 of file NPSMEFTd6.h.

◆ eVBF_1314_DHB

double NPSMEFTd6::eVBF_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3709 of file NPSMEFTd6.h.

◆ eVBF_1314_DHW

double NPSMEFTd6::eVBF_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3710 of file NPSMEFTd6.h.

◆ eVBF_1314_HB

double NPSMEFTd6::eVBF_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3705 of file NPSMEFTd6.h.

◆ eVBF_1314_Hbox

double NPSMEFTd6::eVBF_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3699 of file NPSMEFTd6.h.

◆ eVBF_1314_HD

double NPSMEFTd6::eVBF_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3704 of file NPSMEFTd6.h.

◆ eVBF_1314_Hd_11

double NPSMEFTd6::eVBF_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3702 of file NPSMEFTd6.h.

◆ eVBF_1314_HG

double NPSMEFTd6::eVBF_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3708 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ1_11

double NPSMEFTd6::eVBF_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3700 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ3_11

double NPSMEFTd6::eVBF_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3703 of file NPSMEFTd6.h.

◆ eVBF_1314_Hu_11

double NPSMEFTd6::eVBF_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3701 of file NPSMEFTd6.h.

◆ eVBF_1314_HW

double NPSMEFTd6::eVBF_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3706 of file NPSMEFTd6.h.

◆ eVBF_1314_HWB

double NPSMEFTd6::eVBF_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 3707 of file NPSMEFTd6.h.

◆ eVBF_2_DeltaGF

double NPSMEFTd6::eVBF_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3683 of file NPSMEFTd6.h.

◆ eVBF_2_DHB

double NPSMEFTd6::eVBF_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3681 of file NPSMEFTd6.h.

◆ eVBF_2_DHW

double NPSMEFTd6::eVBF_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3682 of file NPSMEFTd6.h.

◆ eVBF_2_HB

double NPSMEFTd6::eVBF_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3677 of file NPSMEFTd6.h.

◆ eVBF_2_Hbox

double NPSMEFTd6::eVBF_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3671 of file NPSMEFTd6.h.

◆ eVBF_2_HD

double NPSMEFTd6::eVBF_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3676 of file NPSMEFTd6.h.

◆ eVBF_2_Hd_11

double NPSMEFTd6::eVBF_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3674 of file NPSMEFTd6.h.

◆ eVBF_2_HG

double NPSMEFTd6::eVBF_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3680 of file NPSMEFTd6.h.

◆ eVBF_2_HQ1_11

double NPSMEFTd6::eVBF_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3672 of file NPSMEFTd6.h.

◆ eVBF_2_HQ3_11

double NPSMEFTd6::eVBF_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3675 of file NPSMEFTd6.h.

◆ eVBF_2_Hu_11

double NPSMEFTd6::eVBF_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3673 of file NPSMEFTd6.h.

◆ eVBF_2_HW

double NPSMEFTd6::eVBF_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3678 of file NPSMEFTd6.h.

◆ eVBF_2_HWB

double NPSMEFTd6::eVBF_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 3679 of file NPSMEFTd6.h.

◆ eVBF_78_DeltaGF

double NPSMEFTd6::eVBF_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3697 of file NPSMEFTd6.h.

◆ eVBF_78_DHB

double NPSMEFTd6::eVBF_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3695 of file NPSMEFTd6.h.

◆ eVBF_78_DHW

double NPSMEFTd6::eVBF_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3696 of file NPSMEFTd6.h.

◆ eVBF_78_HB

double NPSMEFTd6::eVBF_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3691 of file NPSMEFTd6.h.

◆ eVBF_78_Hbox

double NPSMEFTd6::eVBF_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3685 of file NPSMEFTd6.h.

◆ eVBF_78_HD

double NPSMEFTd6::eVBF_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3690 of file NPSMEFTd6.h.

◆ eVBF_78_Hd_11

double NPSMEFTd6::eVBF_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3688 of file NPSMEFTd6.h.

◆ eVBF_78_HG

double NPSMEFTd6::eVBF_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3694 of file NPSMEFTd6.h.

◆ eVBF_78_HQ1_11

double NPSMEFTd6::eVBF_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3686 of file NPSMEFTd6.h.

◆ eVBF_78_HQ3_11

double NPSMEFTd6::eVBF_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3689 of file NPSMEFTd6.h.

◆ eVBF_78_Hu_11

double NPSMEFTd6::eVBF_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3687 of file NPSMEFTd6.h.

◆ eVBF_78_HW

double NPSMEFTd6::eVBF_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3692 of file NPSMEFTd6.h.

◆ eVBF_78_HWB

double NPSMEFTd6::eVBF_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 3693 of file NPSMEFTd6.h.

◆ eVBFint

double NPSMEFTd6::eVBFint
protected

Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 3640 of file NPSMEFTd6.h.

◆ eVBFpar

double NPSMEFTd6::eVBFpar
protected

Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 3641 of file NPSMEFTd6.h.

◆ eWH_1314_DeltaGF

double NPSMEFTd6::eWH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 3735 of file NPSMEFTd6.h.

◆ eWH_1314_DHW

double NPSMEFTd6::eWH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 3734 of file NPSMEFTd6.h.

◆ eWH_1314_Hbox

double NPSMEFTd6::eWH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 3729 of file NPSMEFTd6.h.

◆ eWH_1314_HD

double NPSMEFTd6::eWH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 3731 of file NPSMEFTd6.h.

◆ eWH_1314_HQ3_11

double NPSMEFTd6::eWH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 3730 of file NPSMEFTd6.h.

◆ eWH_1314_HW

double NPSMEFTd6::eWH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 3732 of file NPSMEFTd6.h.

◆ eWH_1314_HWB

double NPSMEFTd6::eWH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 3733 of file NPSMEFTd6.h.

◆ eWH_2_DeltaGF

double NPSMEFTd6::eWH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).

Definition at line 3719 of file NPSMEFTd6.h.

◆ eWH_2_DHW

double NPSMEFTd6::eWH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).

Definition at line 3718 of file NPSMEFTd6.h.

◆ eWH_2_Hbox

double NPSMEFTd6::eWH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).

Definition at line 3713 of file NPSMEFTd6.h.

◆ eWH_2_HD

double NPSMEFTd6::eWH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).

Definition at line 3715 of file NPSMEFTd6.h.

◆ eWH_2_HQ3_11

double NPSMEFTd6::eWH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).

Definition at line 3714 of file NPSMEFTd6.h.

◆ eWH_2_HW

double NPSMEFTd6::eWH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).

Definition at line 3716 of file NPSMEFTd6.h.

◆ eWH_2_HWB

double NPSMEFTd6::eWH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).

Definition at line 3717 of file NPSMEFTd6.h.

◆ eWH_78_DeltaGF

double NPSMEFTd6::eWH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 3727 of file NPSMEFTd6.h.

◆ eWH_78_DHW

double NPSMEFTd6::eWH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 3726 of file NPSMEFTd6.h.

◆ eWH_78_Hbox

double NPSMEFTd6::eWH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 3721 of file NPSMEFTd6.h.

◆ eWH_78_HD

double NPSMEFTd6::eWH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 3723 of file NPSMEFTd6.h.

◆ eWH_78_HQ3_11

double NPSMEFTd6::eWH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 3722 of file NPSMEFTd6.h.

◆ eWH_78_HW

double NPSMEFTd6::eWH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 3724 of file NPSMEFTd6.h.

◆ eWH_78_HWB

double NPSMEFTd6::eWH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 3725 of file NPSMEFTd6.h.

◆ eWHint

double NPSMEFTd6::eWHint
protected

Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 3642 of file NPSMEFTd6.h.

◆ eWHpar

double NPSMEFTd6::eWHpar
protected

Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 3643 of file NPSMEFTd6.h.

◆ eZH_1314_DeltaGF

double NPSMEFTd6::eZH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3774 of file NPSMEFTd6.h.

◆ eZH_1314_DHB

double NPSMEFTd6::eZH_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3772 of file NPSMEFTd6.h.

◆ eZH_1314_DHW

double NPSMEFTd6::eZH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3773 of file NPSMEFTd6.h.

◆ eZH_1314_HB

double NPSMEFTd6::eZH_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3769 of file NPSMEFTd6.h.

◆ eZH_1314_Hbox

double NPSMEFTd6::eZH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3763 of file NPSMEFTd6.h.

◆ eZH_1314_HD

double NPSMEFTd6::eZH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3768 of file NPSMEFTd6.h.

◆ eZH_1314_Hd_11

double NPSMEFTd6::eZH_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3766 of file NPSMEFTd6.h.

◆ eZH_1314_HQ1_11

double NPSMEFTd6::eZH_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3764 of file NPSMEFTd6.h.

◆ eZH_1314_HQ3_11

double NPSMEFTd6::eZH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3767 of file NPSMEFTd6.h.

◆ eZH_1314_Hu_11

double NPSMEFTd6::eZH_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3765 of file NPSMEFTd6.h.

◆ eZH_1314_HW

double NPSMEFTd6::eZH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3770 of file NPSMEFTd6.h.

◆ eZH_1314_HWB

double NPSMEFTd6::eZH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 3771 of file NPSMEFTd6.h.

◆ eZH_2_DeltaGF

double NPSMEFTd6::eZH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3748 of file NPSMEFTd6.h.

◆ eZH_2_DHB

double NPSMEFTd6::eZH_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3746 of file NPSMEFTd6.h.

◆ eZH_2_DHW

double NPSMEFTd6::eZH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3747 of file NPSMEFTd6.h.

◆ eZH_2_HB

double NPSMEFTd6::eZH_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3743 of file NPSMEFTd6.h.

◆ eZH_2_Hbox

double NPSMEFTd6::eZH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3737 of file NPSMEFTd6.h.

◆ eZH_2_HD

double NPSMEFTd6::eZH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3742 of file NPSMEFTd6.h.

◆ eZH_2_Hd_11

double NPSMEFTd6::eZH_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3740 of file NPSMEFTd6.h.

◆ eZH_2_HQ1_11

double NPSMEFTd6::eZH_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3738 of file NPSMEFTd6.h.

◆ eZH_2_HQ3_11

double NPSMEFTd6::eZH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3741 of file NPSMEFTd6.h.

◆ eZH_2_Hu_11

double NPSMEFTd6::eZH_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3739 of file NPSMEFTd6.h.

◆ eZH_2_HW

double NPSMEFTd6::eZH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3744 of file NPSMEFTd6.h.

◆ eZH_2_HWB

double NPSMEFTd6::eZH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 3745 of file NPSMEFTd6.h.

◆ eZH_78_DeltaGF

double NPSMEFTd6::eZH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3761 of file NPSMEFTd6.h.

◆ eZH_78_DHB

double NPSMEFTd6::eZH_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3759 of file NPSMEFTd6.h.

◆ eZH_78_DHW

double NPSMEFTd6::eZH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3760 of file NPSMEFTd6.h.

◆ eZH_78_HB

double NPSMEFTd6::eZH_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3756 of file NPSMEFTd6.h.

◆ eZH_78_Hbox

double NPSMEFTd6::eZH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3750 of file NPSMEFTd6.h.

◆ eZH_78_HD

double NPSMEFTd6::eZH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3755 of file NPSMEFTd6.h.

◆ eZH_78_Hd_11

double NPSMEFTd6::eZH_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3753 of file NPSMEFTd6.h.

◆ eZH_78_HQ1_11

double NPSMEFTd6::eZH_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3751 of file NPSMEFTd6.h.

◆ eZH_78_HQ3_11

double NPSMEFTd6::eZH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3754 of file NPSMEFTd6.h.

◆ eZH_78_Hu_11

double NPSMEFTd6::eZH_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3752 of file NPSMEFTd6.h.

◆ eZH_78_HW

double NPSMEFTd6::eZH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3757 of file NPSMEFTd6.h.

◆ eZH_78_HWB

double NPSMEFTd6::eZH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 3758 of file NPSMEFTd6.h.

◆ eZHint

double NPSMEFTd6::eZHint
protected

Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 3644 of file NPSMEFTd6.h.

◆ eZHpar

double NPSMEFTd6::eZHpar
protected

Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 3645 of file NPSMEFTd6.h.

◆ FlagFlavU3OfX

bool NPSMEFTd6::FlagFlavU3OfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.

Definition at line 3906 of file NPSMEFTd6.h.

◆ FlagHiggsSM

bool NPSMEFTd6::FlagHiggsSM
private

A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.

Definition at line 3908 of file NPSMEFTd6.h.

◆ FlagLeptonUniversal

const bool NPSMEFTd6::FlagLeptonUniversal
private

An internal boolean flag that is true if assuming lepton flavour universality.

Definition at line 3916 of file NPSMEFTd6.h.

◆ FlagLoopH3d6Quad

bool NPSMEFTd6::FlagLoopH3d6Quad
private

A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.

Definition at line 3910 of file NPSMEFTd6.h.

◆ FlagLoopHd6

bool NPSMEFTd6::FlagLoopHd6
private

A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.

Definition at line 3909 of file NPSMEFTd6.h.

◆ FlagPartialQFU

bool NPSMEFTd6::FlagPartialQFU
private

A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.

Definition at line 3905 of file NPSMEFTd6.h.

◆ FlagQuadraticTerms

bool NPSMEFTd6::FlagQuadraticTerms
private

A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.

Definition at line 3903 of file NPSMEFTd6.h.

◆ FlagQuarkUniversal

const bool NPSMEFTd6::FlagQuarkUniversal
private

An internal boolean flag that is true if assuming quark flavour universality.

Definition at line 3922 of file NPSMEFTd6.h.

◆ FlagRotateCHWCHB

bool NPSMEFTd6::FlagRotateCHWCHB
private

A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.

Definition at line 3904 of file NPSMEFTd6.h.

◆ FlagUnivOfX

bool NPSMEFTd6::FlagUnivOfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).

Definition at line 3907 of file NPSMEFTd6.h.

◆ g1_tree

double NPSMEFTd6::g1_tree
protected

The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).

Definition at line 3810 of file NPSMEFTd6.h.

◆ g2_tree

double NPSMEFTd6::g2_tree
protected

The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).

Definition at line 3811 of file NPSMEFTd6.h.

◆ GammaHTotR

double NPSMEFTd6::GammaHTotR
protected

NP contributions and Total to Higgs width ratio with SM.

Definition at line 3841 of file NPSMEFTd6.h.

◆ gZdL

double NPSMEFTd6::gZdL
protected

Definition at line 3816 of file NPSMEFTd6.h.

◆ gZdR

double NPSMEFTd6::gZdR
protected

The tree level value of the \(Z\bar{d}d\) couplings in the SM.

Definition at line 3816 of file NPSMEFTd6.h.

◆ gZlL

double NPSMEFTd6::gZlL
protected

Definition at line 3814 of file NPSMEFTd6.h.

◆ gZlR

double NPSMEFTd6::gZlR
protected

The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.

Definition at line 3814 of file NPSMEFTd6.h.

◆ gZuL

double NPSMEFTd6::gZuL
protected

Definition at line 3815 of file NPSMEFTd6.h.

◆ gZuR

double NPSMEFTd6::gZuR
protected

The tree level value of the \(Z\bar{u}u\) couplings in the SM.

Definition at line 3815 of file NPSMEFTd6.h.

◆ gZvL

double NPSMEFTd6::gZvL
protected

The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.

Definition at line 3813 of file NPSMEFTd6.h.

◆ Lambda_NP

double NPSMEFTd6::Lambda_NP
protected

The new physics scale [GeV].

Definition at line 3634 of file NPSMEFTd6.h.

◆ lambdaH_tree

double NPSMEFTd6::lambdaH_tree
protected

The SM tree level value of the scalar quartic coupling in the potential.

Definition at line 3826 of file NPSMEFTd6.h.

◆ LambdaNP2

double NPSMEFTd6::LambdaNP2
protected

The square of the new physics scale [GeV \(^2\)].

Definition at line 3791 of file NPSMEFTd6.h.

◆ lambZ

double NPSMEFTd6::lambZ
protected

Independent contribution to aTGC.

Definition at line 3798 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars

const int NPSMEFTd6::NNPSMEFTd6Vars = 400
static

The number of the model parameters in NPSMEFTd6.

 

Definition at line 759 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars_LFU_QFU

const int NPSMEFTd6::NNPSMEFTd6Vars_LFU_QFU = 204
static

The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.

 

Definition at line 777 of file NPSMEFTd6.h.

◆ NPSMEFTd6M

Matching<NPSMEFTd6Matching,NPSMEFTd6> NPSMEFTd6::NPSMEFTd6M
mutableprotected

Definition at line 3427 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars

const std::string NPSMEFTd6::NPSMEFTd6Vars
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.

Definition at line 765 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6Vars_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.

Definition at line 784 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot

const std::string NPSMEFTd6::NPSMEFTd6VarsRot
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.

Definition at line 771 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6VarsRot_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.

Definition at line 791 of file NPSMEFTd6.h.

◆ sW2_tree

double NPSMEFTd6::sW2_tree
protected

The square of the tree level values for the sine of the weak angle.

Definition at line 3808 of file NPSMEFTd6.h.

◆ sW_tree

double NPSMEFTd6::sW_tree
protected

The tree level values for the sine of the weak angle.

Definition at line 3806 of file NPSMEFTd6.h.

◆ UevL

double NPSMEFTd6::UevL
protected

The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)

Definition at line 3818 of file NPSMEFTd6.h.

◆ v2

double NPSMEFTd6::v2
protected

The square of the EW vev.

Definition at line 3800 of file NPSMEFTd6.h.

◆ v2_over_LambdaNP2

double NPSMEFTd6::v2_over_LambdaNP2
protected

The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).

Definition at line 3801 of file NPSMEFTd6.h.

◆ VudL

double NPSMEFTd6::VudL
protected

The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)

Definition at line 3819 of file NPSMEFTd6.h.

◆ w_WW

gsl_integration_cquad_workspace* NPSMEFTd6::w_WW
private

Gsl integral variable

Definition at line 3924 of file NPSMEFTd6.h.

◆ Yukb

double NPSMEFTd6::Yukb
protected

SM d-quark Yukawas.

Definition at line 3838 of file NPSMEFTd6.h.

◆ Yukc

double NPSMEFTd6::Yukc
protected

Definition at line 3837 of file NPSMEFTd6.h.

◆ Yukd

double NPSMEFTd6::Yukd
protected

Definition at line 3838 of file NPSMEFTd6.h.

◆ Yuke

double NPSMEFTd6::Yuke
protected

Definition at line 3836 of file NPSMEFTd6.h.

◆ Yukmu

double NPSMEFTd6::Yukmu
protected

Definition at line 3836 of file NPSMEFTd6.h.

◆ Yuks

double NPSMEFTd6::Yuks
protected

Definition at line 3838 of file NPSMEFTd6.h.

◆ Yukt

double NPSMEFTd6::Yukt
protected

SM u-quark Yukawas.

Definition at line 3837 of file NPSMEFTd6.h.

◆ Yuktau

double NPSMEFTd6::Yuktau
protected

SM lepton Yukawas.

Definition at line 3836 of file NPSMEFTd6.h.

◆ Yuku

double NPSMEFTd6::Yuku
protected

Definition at line 3837 of file NPSMEFTd6.h.


The documentation for this class was generated from the following files: